UNITED STATES DEPARTMENT OF COMMERCE • Luther H. Hodges, Secretary

NATIONAL BUREAU OF STANDARDS • A. V. Astin, Director

Line Parameters and Computed Spectra

for Water Vapor Bands at 2.7^

David M. Gates, Robert F. Calfee, David W. Hansen, and W. S. Benedict

This work was supported by the Advanced Research Projects Agency under

contract number 250-61: code number 7400-DO.

National Bureau of Standards Monograph 71

Issued August 3, 1964

For sale by the Superintendent of Documents, U.S. Government Printing Office Washington, D.C., 20402 - Price ?2.00
N3t!on?!! Bms'A of Standards

Library of Congress Catalog Card Number: 63-62353
Foreword

Knowledge concerning the infrared transmittance properties of the atmosphere is important to the study of the radiative balance of the atmosphere,

astronomical observation, missile detection and tracking, laser communication,

satellite weather reconnaissance, and optical communication. This Monograph is one of a series intended to provide fundamental information required

for the estimation and interpretation of atmospheric transmittance at infrared

frequencies.

Part I of this Monograph presents the fundamental properties of the 2.7m

water vapor band in terms of line absorptions and the integrated transmittance

at any frequency for infinite resolution.

Part II presents examples of the "degraded" transmittance for finite

resolution, as a function of the spectral slit width, concentration, and pressure

with which direct observations may be compared.

A. V. AsTiN, Director.

Ill
Contents

Part I Page

1. Introduction v

2. Line positions vi

3. Line strengths and half-widths vii

4. Discussion viii

5. References vm

Part II

1. Introduction 85

2. Transmission 86

3. Computational procedure 86

4. Degraded spectra 87

5. References 88

IV
Line Parameters and Computed Spectra for Water

Vapor Bands at 2.^

Part I. Line Positions, Strengths, and Half-Widths

for Water Vapor Bands i/„ 2 z/„ and in the Interval

2857 to 4444 cm ^

David M. Gates, Robert F. Calfee, David W. Hansen, and W. S. Benedict^

The spectral line positions, strengths and half-widths of the vi, 2 v.2, and V3 bands constituting the 2.7 M region of water vapor are presented for the range 2857-4444 cm~i. Lines

attributed to the H2O" and H2OI' molecules in this region have also been calculated and

included along with the "hot hnes" produced by 030-010, 011-010, and 110-010 transitions.

The computations were carried out for values of J through 15.

1. Introduction

It has been evident for many years that the

only fundamental approach to atmospheric transmission problems at infrared frequencies would

be through an understanding of the complete

detailed spectrum, band for band and line for

line. However, the enormous complexity of this

procedure has deterred many investigators from

this approach. The problem is further complicated by the fact that the strength (intensity)

and half-width of each line is dependent upon

temperature and pressure as well as being dependent upon the concentration of the absorbing

gas. Faced with the need to intercompare

various spectroscopic observations of atmospheric

transmission at infrared frequencies, both at low

resolution and at high resolution, it became

evident that one had to tackle the problem of

computing the positions, strengths, and halfwidths of all of the spectral lines within any

region of the spectrum. It would be possible, at

least in principle, to compute the integrated effect

of all these lines on the transmission at any given

position in the spectrum.

Two absorbing constituents, which are of

greatest importance for atmospheric transmission

problems in the infrared region of the spectrxun,

are water vapor and carbon dioxide. It was

decided to work with water vapor first and to

analyze the broad absorption region around 2.7m,

which involves the bands V3, vi, and 2v2. The

many excellent experimental observations and

analyses which have now been made of the water

vapor spectrum, coupled with computations of

line width and intensity, make it possible to

systematically undertake such a program. Furthermore, the advent of the large computer

makes the task of computing the transmission

for given atmospheric conditions a manageable

problem.

The water vapor molecule possesses a very

complicated spectrum with irregularly spaced

lines. It is triatomic, has three normal modes of

vibration, and possesses three very different

moments of inertia, hence falling into the category

known as asymmetric top rotators. The general

theory concerning such a molecule is to be found

fuUy discussed by Herzberg [1954]. The analytical formulation of the rotational structure

of H2O is well known [Mecke, 1933; Randall,

Dennison, Ginsburg, and Weber, 1937; and

Benedict and Plyler, 1951], and will not be re- peated here.

The strong, broad absorption region around

2.7m is caused by the following vibrations: vz, a

strong stretching fundamental with the change of

dipole moment during the vibration along the

least axis of inertia, giving rise to a type A band

with the origin at 3755.92 cm~i; vi, a weaker

stretching fundamental with the change of dipole

moment along the intermediate axis of inertia

(type B band), with the origin at 3657.08 cm~^;

and 2 vi, the first overtone of the bending fundamental (type B band) with the band origin at

3151.60 cm~i. The relative intensities of these

V
bands are approximately ^3 >i : 21-2=120 : 12 : 1. In addition there are lines due to bands of isotopic

configurations of HjO whose normal abundances

are H^O^^, 0.20 percent; HzO^^ 0.037 percent; and

HDO, 0.027 percent. Lines are also due to

bands in which the lower level is vibrationally

excited. At atmospheric temperatures, <320 °K,

the only such level which must be considered is the lowest, V2, and its abundance is very small,

0.033 percent at 287 °K.

In this note we will present a tabulation of the

relevant parameters; frequency, strength, width

and lower-level energy, for all water-vapor lines

which can make significant contributions to afcmos2. Line

Table I contains a listing in order of frequency

of approximately 4500 lines giving their position

(cm~i), intensity (cm~Vg cm"^), half-width

(cm~Vatm), rotational identification for upper and

lower states, energy of the lower state (cm~^),

rotational transition strength, and band designation. The positions of the lines as tabulated here

are computed from the energy levels. The energy

levels in tmn are derived from observed line

positions. All lines observed either in the solar

spectrum [Benedict, 1955 and 1957], or in laboratory spectra [Plyler and Tidwell, 1957 and

Gloersen, 1956], with the exception of a few very

weak lines, are accounted for. It is possible to

predict weaker lines that have not been observed

due to insufficient resolving power under the

proper conditions. These weak lines fall into

several categories. Some of them are transitions

of low inherent probability between levels whose

energies have been established from several observed lines of higher probability. For these the

line position can be predicted to within ±0.05

cm~\ since the ground state energy levels are known to within this limit. We have, however,

also included lines whose positions are much less

certain, involving transitions between higher

energy states, observed weakly or inferred by

extrapolation of one or two lines in observed series.

Most of the lines attributed to HzO'* and

also have not been observed, but their positions

should be calculable to within ±2 cm~i, using for

the rotational energy shifts tabulated

[Benedict, 1957], and the following vibrational

shifts:

i'3= — 15.3 cm-i; ^1=— 7.4 cm-i; 2 V2= — 12.5 cm-i.

The values of H20^® energy levels used in

constructing table I do not difi^er greatly from

those previously published [Benedict 1957],

but are believed to be more self-consistent, the

ground-state levels being based on more recent

precise observations [Rao et al., 1962; Delbouille

et al., 1963]. They also include higher levels

than previously published, the intention being

to include an entry for all levels, even if dubious,

that would lead to transitions whose strength at

pheric absorption between 2857-4444 cm~^ (3.5-

2.25m)- In the "windows" beyond these limits

there is a small contribution from very weak lines

belonging to the three principal bands, however

the main contribution to the weak water vapor

absorption in the "windows" is due to other

bands. At the lower frequency side the vi band

of HDO predominates (i/o=2723.66 cm-i), while

at the high frequency side the weak absorption

is due to 3 fz (j'o=4666.72 cm~0- Because of their

extreme weakness, the information concerning

these bands is not as extensive as those treated in

this paper.

Positions

287 °K is greater than 10~^ cm~Vg cm~^; in

the most completely analyzed band, v^, the strengths

extend to 10"^ cm~Vg cm~^. The upper state

levels may be found from the table by adding

the value of the line position in the first column

to the lower energy state in the E" column.

The notation used to designate the rotational

states of the asymmetric rotator [King et al., 1943]

is J Ka Kc, where Ka and Kc run from 0 to J.

J is the rotational quantum number of total

angular momentum; Ka and Kc are indices that

in the limiting case of the symmetric rotator would

become the quantum numbers associated with the

angular momentum of the molecule about A

and C axes, respectively. The other notation

in common use is Jr, where T=Ka—Kc- The

selection rules for the asymmetric top molecule

are given as foUows:

AJ"=0, ±1

Axis of Dipole Moment Allowed Transition

KaKc KaK,

A (least) e e < > e 0

0 0 < > 0 e B (intermediate) e e

< > 0 0

e 0 < > 0 e

e = even, 0 = odd.

Hence, it is seen from the selection rules for type

A bands AKa^^^c is odd and for type B bands

AKa—AKc is even. The energy levels for the four vibrational

states for each rotational level J KaKc were punched on cards. A computer program was

devised to select the correct transitions in terms

of the selection rules just given. The line positions were calculated for each of the three bands

by subtracting the energy value of the ground

state from that of each of the upper states. These are the line positions in cm~^ listed in the

first column of table I. The quantum number identifications of the

upper and lower states are given in columns 4

and 5. Each column contains the J, Ka, and Kc

values in that order. The sixth column lists the

ground state energy value in cm~^

VI
3. Line Strengths and Half-Widths

The intensity of every line in a rotationvibration band, assuming no interaction effects

between vibration and rotation, may be written

as the product of a vibrational factor, S„, common

to all lines in the band and a rotational factor

Sr, for the particular rotational transition involved.

It is customary to define Sv as the sum of all the

transitions in the band so that

where Qr is the rotational partition function

given by

Qr=^i2j+1) g exp {-E"/kT)

J

where gr is a statistical weighting factor depending

upon the symmetry of the level, and E" is the

ground level energy. The values of g are: g=l for even r"

^=3 for odd r"

where T=Ka—Kc. The value of Qr is evaluated

to be 167.7 at a temperature of 287°K and varies

with temperature approximately with T^"^. The rotational line strength, Sr is:

Sr=L-g-exp i-E"lkT)

where L is called the rotational transition strength,

defined to be the sum of the squares of the magnitude of the direction cosine matrix elements

evaluated for the asymmetric rotator.

A full discussion of how L is evaluated for the

rigid as3anmetric rotator has been given by Cross,

Hainer, and King [1944]. Very useful tables of L

as a function of the asymmetry parameter have

be<5n computed by Schwendeman and Laurie

[1958] for all transitions up to J<12 at intervals

of 0.1 in K, and by Wacker and Pratto [1963] for

higher at a slightly coarser interval in k. For

the ground state of H2O, k= ^^ A—C

^" ^

—0.4377. It is slightly different from that value in

the three excited vibrational states considered

here. We have calculated L by interpolation to

K= —0.4377. The resulting values appear in the

seventh column of table I. It is recognized that

this results only in a first approximation to the

true line strength ; in addition to the neglect of the

changed k in the upper state, other interaction

effects may be expected to enter. Their importance will be discussed shortly.

The values used for Sv in the present computation were as follows:

V3, 5'„=2.63X105 cm-i/g cm-^

f,, 5'. =2.7X10* cm-i/g cm-2

2 V2, S, =2.2\XW cm-i/g cm-2.

The value for V3 is believed to be the most reliable

it is based on a recent determination, Jaffe and

Benedict [1963], of the strength of a well resolved

line near the band center by the dispersion

method and agrees well with other measurements

of the total band absorption. The values for vi and 2v2 are based on intercomparisons of the

relative strengths of lines of the three bands,

principally in the region 3250-3500 cm~i. Some

confirmation of the estimate for 2vi may be

obtained from the low resolution studies of Burch

and Williams [1960] for the low-frequency portion

of the band which is free from overlapping by vi. The value for vi is the least certain, particularly

as this relatively weak fundamental vibration

appears to show interaction effects similar to those

encountered in i'2, with lines in the high frequency

branches showing decreases in strength, and those

in the low frequency branches showing increases.

The general theory for these effects suggests that

a number of processes may be acting in combination so that it is difficult to make a calculation.

The dominant processes in vi would appear to be

interaction with the pure rotation (permanent

dipole moment), increasing principally with rotation about A axis, and Coriolis coupling of the vi and vz vibrations. In the present computation,

no attempt was made to correct for these general

effects. This may result in an overestimate of

many of the high J lines in the high frequency

branches by factors of 200 to 300 percent, and in

underestimates of the highest J lines in the low

frequency branches by 50 to 100 percent.

The interaction effects do not appear to be large

in 2v2, except possibly in some of the weaker

branches, such as P31.

In V3, present indications are that interaction

effects do not have a noticeable influence on the

high L lines of the Eqi and Poi branches, although

experimental confirmation would be desirable.

However, some of the weaker branches appear to

show interaction effects [Benedict, 1955]; in particular the Qii, and Q32, and Q43 branches are increasingly weaker than calculated. In addition

to the general interaction effects just mentioned,

there are instances of accidental perturbation when

lines from a common lower state to upper state

levels of the same J in different bands lie close

together. In these cases the weaker line, usually

in Vi, "borrows" strength from the stronger, line.

For these cases the values of L have been adjusted

so that the total strength remains constant, but

shared in a desirable proportion. In the table

such enhanced lines are designated "-(-" at the

right margin. The "lending" line is designated

Although the rigid line strengths may be in some

cases uncertain for the reasons outlined, it is hoped

that their publication in this form will be useful.

Comparison of the composite transmission spectra

derived from table I in various spectral regions

with observed transmission spectra at various pres- sures and temperatures, and further measurements

VII
of the absolute or relative strength of well-resolved

lines, should reveal whether systematic deviations

exist. If so, these may be accounted for by variations in Sv, or introduction of empirical or theoretical factors with the correct rotational dependence on the several bands.

Values of the half width of the lines are listed

in column 3, table I of this paper. The halfwidths for the vi and 21^2 lines were taken directly

from the body of the tables published by Benedict

and Kaplan [1959]; the half-widths for the V3 lines were calculated from the average half width, 7, as given in the last column of these tables. Estimates for higher J lines not appearing in the tables

by Benedict and Kaplan [1963] were made by

extrapolations of these tables. It should be noted

[Benedict and Kaplan, 1964] that the widths

apply to water vapor in air rather than N2 as implied by Benedict and Kaplan [1959]. The

accuracy of the widths is not known, but recent

measurements [Saiedy, 1961] confirm that they

should be satisfactory for absorption computations.

The band identification is given in the last column of table I. As mentioned, the symbols "-(-"

and " — " denote lines in which the band is mixed

by perturbation. An asterisk indicates a line in

the corresponding band of the isotopic molecule

HjO^*, a double asterisk HjO^^, and three asterisks a "hot" line.

4. Discussion

Line strengths were calculated at 287.7 °K for

all possible transitions in the three principal

bands up to «/max = 15. The strongest line (404-

503 in V3, a.t 3838 cm-i) has <S'=9.23X10^ cm-^/gm

cm~^. Since the purpose of the table is to list all lines of possible significance in atmospheric

transmission problems, the lower limit of S was

set at 10"^ cm~Vg cm~^ in the band wings and

at 10"^ in the central region 3503-3950 cm"^,

which includes all lines with »S'>2X10^. In

addition weak lines were excluded if within 0.25

cm~^ of a strong line whose strength exceeded the

strength of the weak line by 10^ or if within 0.5

cm~i of a strong line whose strength exceeded the

strength of the weak line by 4X10^. This

limitation excludes from the table a large proportion of the lines in the weak branches of the

original bands and in the weak satellite bands

due to H20l^ HjQi^ and the "hot" transitions

011-010, 110-010, 030-010. No attempt was

made to list lines in the vi band of HDO (^0=

3704.25 cm~i) as it was determined that its

strongest lines, with few exceptions, would be

excluded by the above criteria. The very weak

combination bands of HDO, vi-\-v2 (I'd =4100.05

cm~i), and 3 V2, (;^o=4145.59 cm~i), also are not

considered.

It must be emphasized that the exclusion of

extremely weak lines from table I was for purposes

of saving space in printing and time in transmission computations based on line-by-line integrations. The actual distribution in strength of

the lines in the spectrum includes additional

weak lines in the categories mentioned and other

weaker lines of vibrational and rotational states,

which have not been included here. These

higher-state lines are important when considering

the absorptivity or emissivity of water vapor at

elevated temperatures.

5. References

Benedict, W. S. (1955), Comments on a table of solar spectrum wavelengths 11984A to 25578A, O. C. Mohler,

Univ. of Mich. Press. Benedict, W. S. (1957), Comments on the spectra of

telluric H2O and CO2 as observed in the solar spectrum,

2.8-23.7 microns, M4m. Soc. Roy. Sci. Liege, Special

Vol. 2, 18-30.

Benedict, W. S. (1957), Identification of HjO" and

telluric lines in the infrared solar spectrum, M6m. Soc. Roy. Sci. Liege, 4th Series, 18, 557-571.

Benedict, W. S., and L. D. Kaplan (1959), Calculation of

line widths in H2O-N2 collisions, J. Chem. Phys. 30,

338-399

Benidict, W. S., and L. D. Kaplan (1963), Calculation of

water-vapor line widths, self-broadened and 02-broadened, J. Quant. Spect. Rad. Trans. 3 (in press).

Benedict, W. S., and Earle K. Plyler (1951), Absorption

spectrum of water vapor and carbon dioxide in the

region of 2.7 microns, J. Res. NBS 46, 246-265.

Burch, Darrell E., and Dudley Williams (1960), Infrared

absorption by Ti-inor atmospheric constituents, Scientific

RePoU 1 (AFCRL TN-60-674).

Cross, P. C, R. M. Hainer, and G. W. King (1944), The

asymmetric rotor, II. Calculation of dipole intensities

and line classification, J. Chem. Phys. 12, 210-243.

Delbouille, L., G. Roland, M. Migeotte, and J. W. Swensson (1963), A table of solar spectrum wavelengths,

7500-12000 A (private communication).

Gloersen, Per (1956), High resolution spectroscopy in the near infrared, Dissertation, The Johns Hopkins University (80 pp).

Herzberg, G. (1954), Infrared and Raman spectra of polyatomic molecules (632 pp). (Van Nostrand Co., Inc., New York).

JaflFe, J. H., and W. S. Benedict (1963), Strength of 1-3 in H2O. J. Quant. Spect. Rad. Trans. 3, 87-88.

King, G. W., R. M. Hainer, and P. C. Cross (1943), The

asymmetric rotor, I. Calculation and symmetry clas- sification of energy levels, J. Chem. Phys. 11, 27-42.

Mecke, R. (1933), Das Rotationschwingungsspektrum

des Wasserdampfes. I, Z. Physik, 81, 313-335.

Plyler, Earle K., and E. D. Tidwell (1957), The precise

measurement of the infrared spectrum of molecules of

the atmosphere, Mim. Soc. Roy. Sci. Li^ge, 4th Series

18, 426-449.

Randall, H. M., D. M. Dennison, N. Ginsburg, and L. R.

Weber (1937), The far infrared spectrum of water vapor,

Phys. Rev. 52, 160-174.-

Rao, K. Nahahari, W. W. Brim, V. L. Sinnett, and Ralph

H. Wilson (1962), Wavelength calibrations in the infrared IV. Use of a 1000-lines-per-inch Bausch and Lomb

plane rephca grating, J. Opt. Soc. 52, No. 8, 862-865.

Saiedy, F. (1961), Atmospheric observations of line intensity and half-width in the rotational and "2 rotationvibration bands of water vapor, Quart. Roy. Met. Soc.

13, 578-587.

Schwendeman, R. H., and V. W. Laurie (1958), Table of

line strengths for rotational transitions of asymmetric

rotor molecules (Pergamon Press, Ltd., New YorW.

Wacker, Paul F., and Marlene R. Pratto (1963), Micro- wave spectral tables, Vol. II. Line strengths of asymmetric rotors, NBS Mono. 70.
TABLE

PARAMETERS OF THE 2.7/i.

LINE HALF

FREQUENCY STRENGTH WIDTH J' cnn~i cm~l

ymn rY> nr\ ~ C. ciii atm.

C. OOH • J? H 0 . DA ? 3 0 - 0 7 6 Q Rw A

w . w •+ j3 0-037 1 3 1X 1

3

9 ft A7 • QQ . VJ J. ^ 0-037 1 3 0 1

3

£. W f X • ^ (J 0-0804 0-0874 0

0-0018 \J # w w X w 0.0 74'^ 1 5

P 874 - 1 7 0.0019 0.0701 V> • W ( w X 1X 0w 6

0.0062 0.0677 9 4 6

?879 . 7^^ 0.1 306 0 . 0 868 5 1 5

<1 O O i • H ^ 0 00 1 1 0 - 0 ft ft Qy 0 Q7

/I O O H- • O J? 0 - 00 1

4

W # W W X ^ 0.070'^

^ U U ^ # 0.00 29 0.0571 w • w ^ 1 X 1X 0w

£. ij \J 0 ± ±' 0 - 00 73 0.0771 1^ # W 1 (X 5 3 2

? 889 • 1 0.0010 W # W w X w 0.0603 • w w w 1X 0w 5 ^ o y \j m ^ ^ 0 - 04 5 U 0-0374 1X ^7 1 12

P 8 Q 0 - ? 7 0.01 51 0-0375 X ^ 0 X1 7£. ^ O 7 u • o ^ 0 0 0^7 0.0871 A c ^ O 7 t, • ^ 7 0-00^1 0 - 0 R 5 7 —J P ft Q HQ 0 n ? 7 7 0 0 71 1 Q7 A*-r P ft Q A 0 00 %u O . 0 7 A 9 AH"

1X A 780"^ 77 0 -4658 0 . 0 8 3 Q A cp R ^ U 7 U • WW 0 . 00 1

3

w • w w X —

0.0779 VJ • W 1 7 Aw 2 4

^ U 7 O • ^ X 0.01 W • W X ^ Au n . 0 74

1

7 0 7

2897.84 0.0014 w • W X " 0 . 0948 1 3

P ft Q Q . ^9 0 . 00 74 0 . 0 7 7 1 J> 0w 1 3

0 on "?

A

O 0 44 fto 1X RO

9 Q n 1 ft 7 c.y \J L m O £. 0 0 R IS O 0 7 8 9 U • V 1 O c. 7 _?

c.

? 9n ? • R ^ 0 - 004 1 O . 0AA5 Q7 1X Hw 0-079'^ 0U .• DfslA D f O

ftU 4

c2905.98 y \j .J % y \j 0W .004'^ • W W "T" _^ 0 - 0 A84 1X 0w 7

^ 7 U • V-> ^ 0\J » 00W W 3^ 1X 0.061 \J # W W X Al_/ X X

ftU

^ 7 U u • I L 0 ? ft Q nW *• 0w ftCJ QO7 V _? 0w

c.p Qy n\j 7I .* L.? ^D 0-00 \J # w w ^70w 0 * 0 ft A R A c p

7 Q n 7 A '^ 0 00 A 0 n 0 7 A 7 p 2908. 10 0.0035 0.033 13 1 12

2908.42 0.0012 0.033 13 2 12

2910.47 0.0041 0.0569 9 5 5 2910.75 0.0050 0.0733 4 3 2

2911. 34 0.0217 0.0708 8 4 4

2911.40 0,0016 0.0608 5 4 1 2911.57 0.0017 0.0734 4 3 1 2911.90 0.1434 0.0335 11 0 11

2911.95 0.0478 0.0331 11 1 11

2912.00 0.0123 0.0583 9 5 4

2912.26 0.0077 0.0547 8 0 8

BAND OF WATER VAPOR

1" F" 1 BAND

cm~'

9 4 5 1360.28 1.797448 2NU2

14 0 14 2073.66 12.99955 2NU2

14 1 14 2073.66 12.99957 2NU2

5 3 3 504.00 0.095779 2NU2

5 4 2 610.12 0.003573 2NU2

11 5 7 1985.83 3.652101 2NU2

10 5 5 1724.72 3. 272354 2NU2

6 2 4 602.77 0. 254241 2NU2

10 1 10 2705.18 9.013676 2NU2**-*

5 5 0 742.10 0.001850 2NU2

1

1

6 5 2144. 12 4. 582064 2NU2

6 4 3 2398.39 3. 153879 2NU2***

1

1

6 6 2142 .69 4. 667626 2NU2

13 0 13 1806.78 11.99672 2NU2

13 1 13 1806.78 11.99676 2NU2

5 3 2 2130.50 1.841317 2NU2***

6 3 4 2271.70 2.452523 2NU2***

10 5 6 1718 .77 3. 697402 2NU2

4 4 1 488. 10 0.001222 2NU2

7 3 4 842.38 0.996364 2NU2

6 5 1 888 .63 0.010677 2NU2

7 3 4 842 .38 0.033256 2NU2

4 2 2 1922.92 0.610552 2NU2***

13 1 12 2042.33 1.90653 2NU2

9 0 9 2512.36 8.007087 2NU2***

8 4 4 1131 .76 2.323327 2NU2

9 4 5 1360.28 0. 1 16860 2NU2

9 5 4 1477.31 3.682999 2NU2

11 4 8 1843.02 4.032477 2NU2

12 4 9 2124.98 4.836759 2NU2

4 3 2 382.52 0.051049 2NU2

5 3 3 2126.41 2 .324407 2NU2***

7 5 2 1059.85 0.038149 2NU2

14 2 13 2327.90 11 .01049 2NU2

14 1 13 2327.88 11 .00954 2NU2

10 6 4 1875.53 4.830967 2NU2

5 4 1 2251.86 3.250024 2NU2***

9 5 5 1474.99 3.26 2NU2-

6 5 2 2552.85 4.266963 2NU2***

5 4 2 2251.71 3.270203 2NU2^**

12 1 12 1557.91 11 .021891 2NU2

12 0 12 1557.91 11.021861 2NU2

10 6 5 1875 .00 4.857731 2NU2

9 5 5 1474.99 0.0557 NU1 +

1
LINE HALF

FREQUENCY STRENGTH WIDTH J' K J" K E" L BAND

cm~i

gm cm~2 otm.

2913.06 0.0019 0.0481 10 6 5 11 7 4 2321 .94 5.877228 2NU2

2913.26 0.0407 0.0737 9 3 6 10 4 7 1581 .34 3.465920 2NU2

2914.^8 0.0019 0.0653 7 1 6 8 2 7 2495.18 4.996649 2NU2***

2917.36 0.0019 0.0712 8 2 6 8 5 3 1255.92 0.098024 2NU2

2919.00 0.0055 0.0534 7 0 7 8 1 8 2337.70 7.000291 2NU2***

2919. 58 0 .0410 0.0775 8 3 5 9 4 6 1340.89 3. 141455 2NU2

2920.90 0.0035 0.0858 3 2 2 4 3 1 2005.92 2. 164905 2NU2***

2921 . 33 0.0018 0.0542 7 1 7 8 0 8 2337.53 6.998008 2NU2***

2921.39 0.0013 0.0764 6 1 5 7 2 6 2318.53 4.008107 2NU2***

2922.00 0.0036 0.0688 9 2 7 9 5 4 1477 .31 0. 180415 2NU2

2922.33 0.0083 0.0337 12 1 12 12 2 11 1774.74 1.854861 2NU2

2922.45 0.0028 0.0337 12 0 12 12 1 11 1774.60 1.854934 2NU2

2923. 10 0 .0027 0.0920 4 1 4 5 2 3 446. 50 0.386397 2NU2*

2923. 16 0.0017 0.0776 6 3 4 7 4 3 931.22 2.767638 2NU2*-

2924.62 0.0400 0.0338 12 1 11 13 2 12 2042.38 8.71329 NUl

2925.25 0.0128 0.0349 12 2 11 13 1 12 2042.33 9.99731 2NU2

2925.38 0.0011 0.0864 5 2 4 6 3 3 661.56 1.411171 2NU2*

2926.46 0.0112 0.0851 3 2 1 4 3 2 2004.81 2.320352 2NU2***

2928.70 0.0065 0.0842 5 1 4 6 2 5 2161 .30 3. 129447 2NU2***

2930. 16 0.3523 0.0796 7 3 4 8 4 5 1122.72 3.022183 2NU2

2930.54 0.0787 0.0665 7 4 4 8 5 3 1255.92 3.953657 2NU2

2931.10 0.0054 0.0709 8 1 7 8 4 4 1 131 .76 0. 146118 2NU2

2933. 14 0.1399 0.0354 10 0 10 11 1 11 1327. 14 10.018239 2NU2

2933. 18 0.2406 0.0686 7 4 3 8 5 4 1255. 16 4.002077 2NU2

2933.26 0.4196 0.0348 10 1 10 1

1

0 11 1327.14 10.018153 2NU2

2933.69 0.0464 0.0557 8 5 4 9 6 3 1631.41 5.006530 2NU2

2933.73 0.8408 0.0776 6 3 4 7 4 3 931 .22 2.767638 2NU2

2934.73 0.0155 0.0565 8 5 3 9 6 4 1631.27 5.013867 2NU2

2935.23 1.3260 0.0920 4 1 4 5 2 3 446.50 0.386397 2NU2

2935.65 0.0032 0.0680 3 3 1 4 4 0 2129.65 3.390390 2NU2***

2935.77 0.0097 0.0683 3 3 0 4 4 1 2129.63 3.393148 2NU2***

2936.00 0.0035 0.0545 4 4 1 5 5 0 2406.15 4.396748 2NU2***

2936.01 0.0012 0.0546 4 4 0 5 5 1 2406. 15 4.397010 2NU2***

2936. 18 0.0058 0.0475 9 6 3 10 7 4 2054.40 6.019433 2NU2

2936.74 0.0343 0.0895 2 0 2 3 3 1 285.23 0.013376 2NU2

2936.82 0.0035 0.0647 6 0 6 7 1 7 2181 .12 5.990506 2NU2***

2936.95 0.5512 0.0864 5 2 4 6 3 3 661 . 56 1.411171 2NU2

2937.48 0.0033 0.0901 4 1 3 5 2 4 2024.17 2.444582 2NU2***

2937.60 0.0019 0.0473 9 6 4 10 7 3 2&54.40 6.018378 2NU2

2938.50 0 .0203 0.0793 6 0 6 6 3 3 661.56 0.051901 2NU2

2939.65 0.0106 0.0950 2 1 2 3 2 1 1819.34 0.925282 2NU2***

2939.66 0.0407 0.0361 11 1 10 12 2 11 1774.74 9.078065 2NU2

2940,92 0.0105 0.0671 6 1 6 7 0 7 2180.65 5.983681 2NU2***

2941 .00 0 .0136 0.0379 11 2 10 12 1 11 1774.60 9.076485 2NU2

2942.48 0.0022 0.0388 9 0 9 10 1 10 1114.56 9.013676 2NU2*

2943.45 0.0112 0.0465 11 2 9 12 3 10 1962.55 7.003088 2NU2

2944.02 0.0025 0.0470 12 3 10 13 2 11 2246.98 7.82232 2NU2

2944.73 0.0097 0.0358 11 1 11 1

1

2 10 1525.13 1 .851690 2NU2

2944.94 0.0291 0.0359 11 0 11 1

1

1 10 1524.87 1.851910 2NU2

2945.75 0.0024 0.0559 8 4 5 9 7 2 1810.63 0.0668 NU1 + 2945.95 0.3158 0.0790 6 3 3 7 4 4 927.77 3.050978 2NU2

2945.98 0.0013 0.0643 6 4 3 7 5 2 1059.85 4. 131192 2NU2^<-

2946.57 0.0134 0.0544 10 2 8 11 3 9 1695.03 5.954956 2NU2

2946.96 0.0018 0.0656 7 0 7 7 1 6 2309.74 1.838288 2NU2***

2
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm~i cm~i

qm cm~2 atm.

2947.61 0.0188 0.0841 2 2

2948.08 0.0415 0.0748 7 1 2948.65 0.0063 0.0830 2 2

2948.89 0.0145 0.0930 3 1 2950.44 0.0056 0.0777 4 1 2951.26 0.0014 0.0795 7 2

2951.38 0.0015 0.0769 5 3

2953.15 0.1143 0.0637 9 2

2953.47 0.0176 0.0771 5 0

2954.17 1.1029 0.0388 9 0

2954.43 0.3677 0.0382 9 1 2955.09 0.0486 0.0787 5 1 2955.28 0.0206 0.0785 6 1 2955.57 0.0424 0.0401 10 1 2955.61 0.6655 0.0643 6 4

2956.02 0.0046 0.0771 5 3

2956.35 0.2225 0.0656 6 4

2956.84 0.0475 0.0537 7 5

2956.97 0.1426 0.0539 7 5

2957.01 0.0981 0.0716 8 2

2958.41 0.1273 0.0442 10 2

2959.78 0.0045 0.0557 11 3

2960.27 0.0037 0.0743 6 1 2960.78 0.0059 0.0806 5 1 2961.38 0.6888 0.0795 7 2

2961.69 0.7464 0.0769 5 3

2962. 11 0.0094 0.0871

4 2

2962.86 0.0017 0.0447 8 0

2963.32 0.0052 0.0443 8 1 2963.42 0.0066 0.0959 2 1 2963.75 0.0214 0.0454 8 6

2964.75 0.0055 0.0454 8 6

2966.00 2.3187 0.0771 5 3

2966.64 0.0037 0.0848 6 2

2966.74 0.0926 0.0393 10 1 2967.24 0.0311 0.0397 10 0

2967.65 0.0062 0.0852 5 2

2967.68 0.0017 0.0871

4 2

2967.91 0.4999 0.0835 6 2

2968.85 0.0086 0.0880

4 0

2969.45 0.3534 0.0463 9 1 2970.17 0.1589 0.0843 5 0

2970.62 0.0011 0.0604 5 4

2970.73 0 .0033 0.0608 5 4

2971.66 0.0014 0.0777 6 0

2972.34 0.0027 0.0948 3 1 2972.80 0.0011 0.0852 5 2

2973.25 4.6875 0.0871

4 2

2974.00 0.0070 0.0947 1 1 2974.63 0.8690 0.0447 8 0

2975.10 2 .6070 0.0443 8 1 2975. 13 0.1186 0.0534 9 2

2977.28 0.0100 0.0733

4 3

2977.30 0.0399 0.0655 10 3

1" 1 BAND

cm~i 1 3 3 0 19 07.63 2. 366160 2NU2*** 6 f 4 3 931 .22 0. 135960 2 INU 2 0 3 3 1 T 0 "J / "7 1907 . 4 r 2 . 394805 2 NU 2

^.4 2 3 1 Q

A "7QQ 1 y 0 ' . y y 1 Q "7AQ /iQ

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Q 1 D f » toAAQ /i 7 '3 9 9 M 1 19 A NU A

y i i 2 1 A 10 i y 5 • 1 3 0 . 06 32 13 9 Ml 19 2NU 2 3 7 5 2 1059.85 4.131 192 2(nU2 2 6 4 3

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C ^ "7C 3.153879 2InU2*

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n ^ R 1 u y • ot> 4. 143 5 y4 2NU2 9 M 1 19 3 Q 6 I 14 i 1 • 60 5.142/11 9 M I 19 2NU2 Q0 6 3 1411 .65 5 . 144364 9 M t 19 2inU2 6 Qy 3 1 Id Lb • d 1

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"7 1 . o4 1 31/ 9 M 1 19^ 2NU 2*

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y 1 y 9/^0.21 0 . 00 '851 2 IN

U 2 * QO y 0 y 20 . 1 0 Q A A "7 A 0 ~7 8 . 00 / 0 0 7 2 NU 2* i 3 2 c. 1 0 i 3 . 8 i 1 . 66666 / 2 InU 2 *** 3 y { c 1010.63 5.53 M 1 1 "> InU2 —

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Qo 1 0 2 Q 1293.66 "7A /. 9 £ 1 / . 043 66 1 9 M 1 1 O 2 NU 2

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C r\ 0 0 1 AA ^ 0 /. ~7 ^ 0 . 06 24 / 6 9 M 1 1 9 A NU 2

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LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm"' cm~i

gm cm~2 atm.

2977.96 3.1032 0.0852 5 2

2978.37 0.0024 0.0839 5 1 2978.45 0.0034 0.0734 4 3

2980.25 0.5431 0.0604 5 ^ 2980.35 1 .6302 0.0608 5 4

2980.75 0.0018 0.0646 8 2

2981. 13 0.3918 0.0498 6 5 2981 .21 0.0255 0.0993 1 1 2981.24 0.1306 0.0499 6 5 2981.36 0.0256 0.0914 4 1 2981.43 0.0041 0.0865 4 2

2982.33 0.0039 0.0653 7 1 2982.38 0.0019 0.0733 4 3

2982.48 0.2942 0.0552 8 1 2982.61 0.0111 0.0534 7 0

2983.22 0.0326 0.0952 3 0

2983. 52 0.0037 0.0542 7 1 2983.87 0.0010 0.0438 12 2

2984.20 1 .3649 0.0948 3 1 2987.49 5 .0028 0.0733 4 3

2987,76 0.0238 0.0422 7 6

2987.76 0.0714 0.0422 7 6

2988. 52 0.0020 0,0534 7 0

2988.58 1 .6807 0.07344 3

2988.60 0.0902 0.0451 9 1 2989.02 0.0012 0,0470 13 1 2989.66 0.2728 0.0459 9 0

2991.43 0 .0760 0.0870

4 0

2991.47 O.OOlO 0.0687 6 1 2991 .93 2 .0331 0.0865 4 2

2992.24 0.0025 0.0764 6 1 2992.64 0 .8868 0.0646 8 2

2992.92 0.0069 0.0858 3 2

2993.68 1 .9468 0.0653 7 1 2994. 13 0.0117 0.0907 4 1 2994.43 5.5317 0.0534 7 0

2995.00 0.0070 0.0545

4

4

2995.01 0.0023 0.05464

4

2995.34 0.0087 0.0871 5 0

2995.38 1 .8446 0.0542 7 1 2996.24 0,0019 0.0447 5 5

2996.38 0.0016 0.0379 11 0

2997.64 0.0119 0. 1006 2 0

2997.70 0.0014 0.0530 8 1 2998, 30 0.0385 0.0747 9 3

2998.37 0.0013 0.0858 3 2

2998.63 0.0032 0.0378 8 7

2998.63 0,0095 0.0378 8 7

2999.08 0,0013 0.0759 7 2

2999.56 0,0225 0.0851 3 2

2999.63 0,0080 0.0531 6 4

2999.82 0,0013 0.0545

4

4

3001.34 0,0129 0.0842 5 1 3001.70 0,0070 0.0647 6 0

J" E"

L BAND

cm~i 3 6 3 4 648 .97 2,452523 2NU2 5 2 2024.1 1 1,711792 2 NU 2*^* i

IT5 4 2 610.12 3,2 / 0203 2NU2* 2 6 5 1 888.63 / 0 ^ y. C "7 /^ 4, 264570 2NU2 1 6 5 2 8 88.60 4, 266963 2NU2 7 9 1 08 1 079 . 07 c n 0 ~7 n 0 0 5,98 ^889 2NU2* 2

-77 6 1 1216. 20 5,265222 2NU2 0 2 2 1 1 742 .28 1 . 500000 2NU2*** 1 7 6 2 1216.20 5 • 265494 2NU2 4 5 0 5 1920.76 3.911752 2 NU2^** 2 5 3 3 504 . 00 T 0 y. y "7 2 . 324407 2NU 2* 6 0 2 7 00 5 . 62 4. 996649 2NU2*

d. 5 4 1 610.3d 3 . 250024 2NU

-7

y 2 00 lOoO . 3o 6,019178 7 Q 1 Q0 ' 44 .16 r ,000291 3 4 1 4 1821.61 3 • 004990 2NU2*** 7 0 0 ' 44 . 09 6,998008 1 i 1 3 3 1 0 2 414. J 3

/-> 0 "7 y. "7 y, 0.2(4^4 iNU 1 3 4 2 2 315.79 0.610552 2NU 2 2 5 4 1 610.35 3.25 0024 2NU2 2 8 7 1 1 590 • 74 6.263414 2 NU2 1 8 7 2 1 590 . 74 6 , 263444 2NU2 7 00 1 8 r 44 .16 1 ,000291 2INU2** 1 5 4 2 610.12 3,270203 2NU2 9 9 2 8 1080.38 1.842036 2NU2 1 2 1 3 2 1 1

2246 • 98 3,76133 2 NU 2 9 9 1 8 1079. 07 1 , 844 131 2NU2 4 4 3 1

r\ r\ y. ~7CO 0 , 04 f 6 52

O Ml 10 2InU2 6 5 4 1 0 • 0005 3 D 2 5 3 3 p04 . 00 2 • 3 

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TM 1 1 n -H. 2INU2* 1 1

12 3 10 1962,55 0,089303 NUl 2 3 1 3 1739,51 2,156792 2NU2*** 8 8 2 7 885.62 1,833129 2NU2* 7 10 2 8 1438.00 4,706625 2NU 2 2 4 3 1 383.85 2 , 164905 T M 1 1 T ^-M. 2NU2** 1 9 8 2 2009.87 7,261219 T M 1 IT 2NU2 2 9 8 1 2009 .87 7,261215 T M 1 IT 2NU2 6 8 1 7 882.93 4,913532 T M 1 IT M. 2NU2* 1 4 3 2 382.52 2,320352 T Kll 1 T 2NU2* 3 7 7 0 1 394 . 86 0.026 MI 11 .i- NU i + 1 5 5 0 742.10 4.396 / 48 4 6 2 5 552,92 3. 129447 2NU2* 6 7 1 7 586,48 5.990506 2NU2*
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ' gm cm~'^ n tm

3002. 14 0,0065 0, 0680 3 3

3002.32 0,0194 0.0683 3 3

3003.26 0,0104 0.0974 3 1 3003.46 1,2588 0.0764 6 1 3003.59 0,0210 0.0671 6 1 3003.80 0,1313 0.0874 3 0

3003.83 3 ,4667 0.0858 3 2

3004.65 3 ,5222 0.0545 4 4

3004.66 1,1741 0.0546 4 4

3004.68 0,0039 0.0783 6 2

3004.89 0,0042 0.0851 3 2

3005,03 0,0060 0.0381 12 2

3005.41 0,3172 0.0447 5 5

3005.41 0,9517 0.0447 5 5

3006.78 0,0024 0.0391 12 1 3006.93 0,0024 0.0842 5 i

3006.95 0,0052 0.0944 3 1 3007.07 0,0014 0.0547 6 4

3007.24 0,0012 0.0680 3 3

3007.42 0,0036 0.0683 3 3

3007.64 0,0013 0.0647 6 0

3009.57 0,0039 0.0671 6 1 3009.66 0,7180 0.0530 8 1 3010.23 11 ,2452 0.0851 3 2

3011,18 0,0067 0.0901 4 1 3011.22 0,6505 0.0759 7 2

3011 .86 0,0023 0.0833 5 2

3011.91 0,2436 0.0548 8 0

3012.24 0,1679 0.0388 6 6

3012.35 3,2325 0.0680 3 3

3012.49 0,0659 0.0388 6 6

3012. 52 6,4740 0.0842 5 1 3012. 52 9,7070 0.0683 3 3

3013. 19 0,0359 0.0621 6 3

3013.47 0,0340 0.1037 1 0

3013. 58 3 ,4942 0.0647 6 0

3014. 14 0,0211 0.0950 2 1 3015. 56 10,4892 0.0671 6 1 3016.22 0,0058 0.0942 4 0

3016.51 0,0092 0.0845 4 2

3016.71 0,0144 0.0955 2 1 3016.76 0,0012 0.0901 4 1 3017,08 0,0027 0.0802 7 1 3017,91 0,0012 0.0634 7 1 3019.35 0,0028 0.0833 3 2

3019,49 0,0074 0.0848 6 2

3019.84 0,0352 0,0771 5 0

3019.89 0,0375 0,0841 2 2

3019,96 0,0039 0,0950 2 1 3020,42 0,0075 0,0947 4 2

3020, 57 0,0084 0.0425 11 2

3021,18 0,0127 0.0830 2 2

3021,94 0,0036 0.0656 7 0

3022,35 3,3500 0.0901 4 1

Kc

I" J

1/ Kc L

1 DMIML/

1 4 4 0 488 .13 3 .390390 2NU2*

0 4 4 1 488 .10 3.393148 2NU2*

3 4 0 4 1817.50 2.831638 2NU2***

5 7 2 6 709.60 4.008107 2NU2

6 7 0 7 586 . 26 5.983681 2NU2*

3 3 3 0 285.43 0.016715 2NU2

2 4 3 1 3o3 . 85 2 . 164905 2NU2

1 5 5 0 742 .10 4. 396748 2NU2

0 5 5 1 742 .10 4,397010 2NU2

5 6 3 4 2271 . 70 2.963539 2NU2'^**

1 4 3 2 382.52 2,320352 2NU2*-»<-

1

1

1 2 3 10 1962,55 3 , 648229 2NU2

1 6 6 0 1045,07 5 , 399693 2NU2

0 6 6 1 1045 , 07 5,399718 2NU2

1

1

1 2 2 10 1960 ,22 3,652921 2NU2

4 6 2 5 552,92 3 , 129447 2NU2**

3 3 2 2 1813,81 1,297651 2NU2***

2 7 7 1 1394,86 0,0133 NU1 +

1 4 4 0 488,13 3,390390 2NU2**

0 4 4 1 488 , 10 3,393148 2NU2**

6 7 1 7 586,48 5 , 990506 2NU2**

6 7 0 7 586.26 5,983681 2NU2**

8 8 2 7 o85 . 62 1,833129 2NU2

1 4 3 2 382.52 2,320352 2NU2

3 5 2 4 416.22 2 , 4445 82 2NU2*

6 8 1 7 882.93 4, 913532 2NU2

4 5 3 3 2126.41 2 , 492 169 2NU2***

8 8 1 7 882.93 1,839778 2NU2

1 7 7 0 1394,86 5 , 44 NU2-

1 4 4 0 488 ,13 3,390390 2NU2

0 7 7 1 1394,86 6 , 40 1 5 18 2NU2

4 6 2 5 552,92 3, 129447 2NU2

0 4 4 1 4o8 , 10 3 , 393 148 2NU2

3 7 7 0 1394,86 0,010200 NU3 +

1 2 1 2 1677.08 1 , 500000 2NU2^**

6 7 1 7 586 .48 5,990506 2NU2

2 3 2 1 212.15 0.925282 2NU2-*^

6 7 0 7 586.26 5.983681 2NU2

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3 4 3 2 2004 .81 1 . 848533 2NU2*-«-*

2 2 1 1 ^42 . 2o 0.833333

3 5 2 4 416.22 2 . 4445 82 2NU2*^

6 7 2 5 2 392.58 3 .983004 2NU2***

7 7 2 6 709.60 1.816721 2NU2*

2 3 3 1 1907.47 1 . 035682 2NU2***

5 7 1 6 704. 22 3.799063 2NU2*

5 6 1 6 447 . 24 4,979001 2i\IU2*

1 3 3 0 28 5.43 2,366160 2NU2*

2 3 2 1 212.15 0,925282 2NU2*^

3 5 1 4 2000 . 90 1,638916 2NU2**-'^

10 1

1

3 9 1695 .03 3,632655 2NU2

0 3 3 1 285.23 2,394805 2NU2*

7 7 1 6 704.22 1,838288 2NU2*

3 5 2 4 416.22 2,444582 2NU2

5
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ~^

U f M 1 1 1 atm.

3022.67 0.2861 0.0834 8 3 6

3023.03 0.0290 0.0930 3 1 2

3023.64 0.0089 0.0835 3 2 1 3023,70 0.0252 0.0445 11 1 10

3023.71 0,0117 0.0806 5 1 5

3025.30 0.0069 0.0841 2 2 1 3025.78 10.5645 0.0950 2 1 2

3026.57 0.0023 0.0830 2 2 0

3026.77 0.0018 0.0653 8 1 8

3027. 10 0.0297 0.0994 2 1 2

3027.14 0.0126 0.0811 10 4 7

3027.72 0.0036 0.0862 4 2 2

3028.55 0.0019 0.0447 11 1 10

3028.66 0.0054 0.0930 3 1 2

3028.71 0.0023 0.0877 6 1 5

3029.75 0.0022 0.0806 5 1 5

3029.87 0.5756 0.0634 7 1 7

3030.72 18.7586 0.0841 2 2 1 3031.27 0.0022 0.0739 6 3 4

3031.74 17.5826 0.0771 5 0 5

3031.75 0.0113 0.0996 0 0 0

3031.93 3.7126 0.0848 6 2 5

3031.96 6.3375 0.0830 2 2 0

3032.42 0.0312 0.0975 3 0 3

3032.88 0.0011 0.0737 5 3 3

3032.98 0.0032 0.0699 4 3 2

3033.49 0.0092 0.0884 5 2 3

3033.63 0.0011 0.0705 4

a

1 3033.76 0.0072 0.0957 2 1 1 3034.29 14.5185 0.0930 3 1 2

3034.37 1 .7979 0.0656 7 0 7

3034.64 0.0033 0.0759 5 3 2

3035. 14 0.0028 0.0340 8 8 1 3035.79 5.8599 0.0806 5 1 5 3036.02 0.0154 0.0912 5 1 4

3036.71 0.0172 0,0880 4 0 4

3036.94 0.0075 0.0743 6 1 6

3037.08 0.0010 0.0927 6 3 4

3037. 12 0.0859 0.0486 10 2 9

3037.54 0.0299 0.0937 3 1 2

3037.63 0.0132 0.0959 2 1 1 3038.73 0.0085 0.0934 4 1 3

3039.07 0.0020 0.0893 6 2 4

3041.25 0.0014 0.0832 7 3 4

3041,30 0.0015 0.0532 11 2 9

3042.33 0.0030 0.0886 7 2 5

3042,67 0.0032 0.0880 4 0 4

3042.70 0.0302 0.0520 10 1 9

3042.75 0.0039 0.0920 5 2 4

3042.92 0.0014 0.0 743 6 1 6

3043.20 0,0020 0.0678 9 3 6

3043.31 0,0024 0.0959 2 1 1 3043.50 0.0146 0. 1021 2 0 2

3044. 14 0.0512 0.0914 4 1 4

1" F" 1 R AMD

cm-1

9 2 7 1201 .95 3 . 529968 2NLI2

4 2 3 300 . 35 1 . 970843 2NU2*

D 3 0 190 ' . 6-5 1.092505 2NU2***

1

1

2 9 1690 • 70 3 . 646421 2NU2

6 0 6 446 .71 4, 958549 2NU2-'^

3 3 0 285.43 2 , 366160 2NU2**

3 2 1 212.15 0,925282 2NU2

3 3 1 285.23 2 . 394805 2NU2**

y 4 5 1360.28 0. 004551 Ml It NU 1 3 0 3 1731.89 1 . 741385 2NU2***

1

1

3 8 1813.26 3. 178818 2NU2

4 3 1 2005 .92 2.167225 2NU2***

1 2 4 9 2 124 .90 0.265959 NU 1 4 2 3 300 .33 1 . 9 ^ 0 843

6 2 4 2 211.21 4. 225862

6 0 6 446 .71 4. 958549 2NU2**

7 2 6 709 . 60 1.816721 2NU2

3 3 0 285 • 43 2. 366160 2NU2

6 4 3 2 398 . 39 1 O ~7 O O C O 2.878858 2 inU 2***

6 1 6 447 . 24 4.9 ^9001 2NU2

1 1 1 1634.97 1 . 000000 2 NU 2***

7 1 6 704.22 3,799063 2NU2

3 3 1 285.23 2 , 394805 2NU2

3 1 2 1 / f 2 .41 2 . 185861

5 4

-> 2 2251.71 2.024051

4 4 1 2129.63 1 . 08 2 946 2 In U * **

5 3 2 2 1 30 . 50 3 . 442901 2NU2***

4 4 0 2129.65 1.08 8294 2NU2^**

2 2 0 1743 .47 1.258755 2NU2***

4 2 3 300,35 1 . 970843 2NU2

7 1 6 704, 22 1.838288 2NU2

5 4 1 2251,86 2 . 066632 2NU2***

9 9 0 2225,56 8 . 403719 2NU2

6 0 6 446 .71 4. 958549 2NU2

5 2 3 2053.98 4. 214107 2NU2***

5 1 5 326.64 3.972803 2NU2*

6 2 5 552 .92 1. /83035

7 2 5 2392 .58 1.512999 2NU2***

1 0 3 8 1446 .16 3 . 60 5 841 T Ml IT 2 NU2

3 2 1 18 19 . 34 2. 538253 2NU2***

3 2 2 206.30 1.666667 2NU2*

4 2 2 1922.92 3 . 6429 13 2NU2***

6 3 3 2 282.59 4. 829435 2NU2***

7 4 3 2572.13 4.268667 2NU2***

1 2 5 8 2275 .44 0. 426841 NUl

7 3 4 2462 .87 5.918411 2NU 2***

5 1 5 326.64 3. V ^ 2803 Z NU

1

0

2

D8 1438 • 00 2NU ^: 6 1 5 542.91 2.671788 0 M 1 1 O 2NU2*

6 2 5 552.92 T ~7 0 0 0 C

1 . 783035 2NU2**

10 6 5 1875.00 0.071662 Mill IMU 1 3 2 2 206.30 1.666667 2NU2**

2 1 1 1693.65 2.074578 2NU2***

5 0 5 325.35 3.911752 2NU2*

6
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ~ ^

g-m cm~2 0 tm.

3044.53 0.0027 0.0777 6 0

3046.20 0.0011 0.0623 7 3

3047.80 0.0010 0.0488 11 2

3048.41 0.0140 0.0947 1 1 3048.64 8.5945 0.0880 4 0

3048.90 3.7332 0.0743 6 1 3048.99 6.5817 0.0959 2 1 3050.04 0.0413 0. 1075 1 0

3050.26 0.0095 0.0914 4 1 3050.67 0.1971 0.0898 7 3

3051.33 0.0024 0.0951 3 2

3051.90 0.0899 0.0563 9 2

3052.47 0.0652 0.0952 3 0

3052.50 0.0069 0. 1044 1 1 3053.80 0.0015 0.0646 8 2

3054.17 0.0026 0.0947 1 1 3054.43 0.0048 0.0839 5 1 3055.34 0.0024 0.0421 10 0

3055.57 0.0511 0.0993 1 1 3055.60 1.9646 0.0920 5 2

3056.38 25.6158 0.0914 4 1 3057. 15 1 .3625 0.0777 6 0

3058.01 0.0011 0.0694 8 3

3058.43 0.0121 0.0952 3 0

3058.45 0.0012 0.0622 10 1 3059.27 0.0019 0.0459 13 2

3059.68 0.0074 0.0440 10 1 3059.93 7.0055 0.0947 1 1 3061.16 0.3016 0.0613 9 1 3061.29 0.0095 0.0993 1 1 3062.61 0.0035 0.0562 9 0

3062.77 0.0111 0.0863 9 4

3064.40 32.6126 0.0952 3 0

3065. 53 0.0209 0.0974 3 1 3065.59 0.7553 0.0646 8 2

3065.85 0.0012 0.0722 7 2

3066.02 0.0036 0.0467 12 3

3066.28 2.3799 0.0839 5 1 3067.01 25.5426 0.0993 1 I 3067.72 0.0237 0. 1006 2 0

3068.43 0.0020 0.0927 6 3

3069.44 0.0149 0.0947 4 2

3069.62 0.0234 0.0907 4 1 3071.73 0.0039 0.0974 3 1 3072.20 0.0107 0.0356 7 7

3072.20 0.0322 0.0356 7 7

3073.18 0.0032 0.0871 5 0

3073.43 0.0042 0.0691 7 3

3073.70 0.0044 0.1006 2 0

3075.50 0.0043 0.0907 4 1 3075.84 0.0078 0.0783 6 2

3076.02 0.0028 0.0947 4 2

3076. 10 0.0018 0.0519 12 2

3076.70 0.0038 0.0617 6 3

J

1/Kc E L BAND

6 6 1 5 542 .91 1.852055 2NU2*

5 8 6 2 1411 .68 0.010619 Mill NU 1 10 1

2

3 9 2105 . 90 0. 278800 Nl 1 1 1 NU 1

1 2 0 136 • 1 / 1 O /. /i "7 /. "7 i • ^:44 * 4 f ^ IN U ^: *

/, 1 Q Q 7 O Q r\ "2

o O ceo Q T 1 7fl O '2 i » 1 O D\J DO 5 Ml 1 ?

i D z

oiL1 A A A ^ A 7 i . Oo O DO f 9 M 1 19 ^ INU c

1 1 1 U

T c; A n A A n 9 M 1 1 9 * * *

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9 M 1 1 9 -li- -it- c Qo 2 O

Q Q O Q T Z • ^ ZZ IQy 9 M I 19

1 3 Lo 1 z> » 49 O.o3boyb A Q "2 A Q 9 M 1 1 9 -If. -IS- -fr A INU A ***

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n

3

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1 1^16.2 ' "2 C C /. A C "7 3 . b b 49 b / 9 M 1 19 ZH\J Z 3 1 4

O A A /i A A A 3. 004990 9 M 1 1 9 -If- A NU A *

i 2: 0 2

1 ^ ^ y. o "7 A "7 C O R "2 0. / bb<db3 9 Ml 1 9 -If- -it -it- A NU A***

( Qo 6 i OOo . 1 <C ^ . M-bOiiyb 9 M 1 1 9 -if- A NU A *

i 2 0 136.1/ 1 . 244 / 4

/

^ NU A**

c

!:> c 2 4 ^16 . 2ii 1 ~7 T T ~7 A O 1. fil I^Z 9 M i 1 9 aNU A*

10 1 i 3 9 169b . 03 A A A "7 O T 1 0.09 '311 Mill NU 1 0 2 i 134.91 1 C A A A A A

1 . bOOOOO aNU 9 Ml 1 9 -M- ^1*

/Io i

C, Dm-^: . y 1 A9 NUM 1 19A

A

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C, a 9 c o t; -3 ^ ~ . 5 -J AINU 9 Ml 1 9A O

/I D i C 1 ft 9 A R 9 M 1 19 A NU A Q 6 '+ A A "2 '5 A /i O Mill NU i 3

14 1 4 224.83 O A A /. A A A

3 . 004990

1

0

Qy 2 ( 1^:01 • y!? A A T C r\ O "7 0»01p02 r O M 1 to 2nU^:

i i 1 3 3 10 ^:M i*f • ^ 3 3 • r 3 3 D 3 aNU^ 9 M 1 19

1 niU i 1 Q 1 D V U • A UA A Q 7 Q "7 O NUM 1 1 1i i

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c. 0

1 ':i T

"7 i 3 D • I 1 T O /i /. ~7 /. "7 1 • ^44 / 4 r 9 M 1 19 aNU A

Qo o

2 1 iilO 1 • y !:? 3«6 { ^cOD 9 M 1 19

r\U

oc I. i X 3m- • V iT A A A A A 9 Ml I 9-tt--5*- A NU A Q Q

c5 3 5 A A 1 A "7 Q 0«Jl->9 / 9 aNU 9 Ml 19A

/: O 1 u 3 1 1 IP 3o • ^1

3

2 • 1 / 164

1

9 M 1 19 A NU Z

i Q A A /i Q Q A 3 • OU 499 0

9 M 1 19 A NU A 0 4 TOO A /:l 2 . o3 163o 9 Ml 1 9 aInU Z*

( Qo 3 O

1 A A A TO

1 (JOo • i ^1 J . boiiy b ANU 9 M 1 19A

6 I 3

Q 1 A "7 O •2 O 7 O y. A o i • Z 1 3499 9 M 1 1 9 -If- A NU A*

i U 1 ^1 Q7

O 1 9 /i Q ft z 1 <i *+ » y O

"2 a 1 1 O aNU 9 Ml I 9A

c b 2 4 M- 16 • 2^ T 7 1 1 7 A O 1. (11 '92 2NU2 9 M 1 19

(J 2 1 Toy. Q 1 1 3h • y

1

T A A A A O

1 • 0000 aNU2 9 Ml 19

2 3 1 3 142 » 2o 2 . 156792 2NU2^

1 2

c5 / o2 . 40 1 C T O A O A 1 . b 1 2999

i

a

1 399 • 46 l»63o916 2NU 2*

1. i. 3 3QU • 3

1 C, ~7 Q A A 1«->D/30U ^ IN U ^ *

0

/, ccc

06 ^:»o3163a

i Qo

Qo 0

~7 /t A O ~7 Q O r #402 Ao3 2NU c 0

Qo

QO i1 "7 Q O 1 A 1 r o V • 10 ~7 /i A O "7 Q '2

f • 40 <i { O D

O MI 1 O

c0 1 4 399 • 46 l«91233o 2NU2**

A- Qo 6 3 1411 %bD 0«013422 Mill NU 1

c. 3 1

1 y* o oft 14<i • 2o Cm iDO / 92

1, H 4 2 3 300 .3b 1.56 (300 2inU 2**

5 6 3 4 648 . 9

/

O A ^ O C O A

2 .963539 M 1 I A Jit 2NU2*

3 5 1 4 399 . 46 1.638916 O M I in ^ vc 2nU2**

10 12 3 9 2105.90 5. 509361 2NU2

4 7 6 1 1216.20 0.004557 NUl

7
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ~^ rm ~ 1

y 1 1 1 LI M

rm ~ 1 ^111 otm.

3076.98 0,0059 C.0528 11 3 9

3077.34 0,0058 0.0753 5 1 4

3077.43 0,6168 0.0722 7 2 6

3077.93 10.4331 0.0974 3 1 3

3078.90 0.0014 0.0711 7 2 5

3079.52 8.7109 0.0871 5 0 5

3079.69 11.8510 0. 1006 2 0 2

3079.95 0.3099 0.0706 8 1 7

3081 . 38 11 .7249 0.0907 4 1 4

3082.03 0.0104 0. 0944 3 1 3

3082.55 1.0167 0.0927 6 3 4

3082 .60 7.4729 0.0947 4 2 3

3083. 17 0.0022 0.0595 10 2 8

3083.33 0,0045 0.0833 5 2 4

3083 . 88 0.0054 0,0802 7 1 6

3083.90 0,0680 0,1037 1 0 1 3085.32 0,0020 0.0445 9 6 4

3086. 07 0,0015 0.0710 9 1 9

3086.30 0,0029 0.0438 12 1 11

3086.66 0,0629 0,0590 10 3 8

3087.15 0,0116 0.0942 4 0 4

3087. lb 3.8873 0.0783 6 2 5

3087,86 0,0019 0.0944 3 1 3

3088.51 0.0184 0.0845 4 2 3

3088.57 0,0594 0.0994 2 1 2

3089.04 0,001

1

0.0794 8 5 4

3089.62 0,0236 0.0684 7 0 7

3089.92 0.0126 0. 1037 1 0 1 3090.05 0.0112 0.0845 4 0 4

3091 .03 0.0011 0.0705 8 3 6

3091 .43 0.0287 0.0955 2 1 2 3091.51 0.0056 0.0833 3 2 2

3091.98 0.0014 0.0663 6 3 3

3092.30 0.0014 0.0597 9 1 8

3092.74 0.0228 0.0614 11 2 9

3093.45 0.0022 0.0942 4 0 4

3093.69 5 . 1996 0, 0944 3 1 3

3094,02 0.0034 0,0845 4 2 3

3094. 51 2 .2546 0.0833 5 2 4

3094, 86 0.0110 0.0994 2 1 2

3095,41 0.0655 0.0651 9 3 7

3095,94 34.0199 0. 1037 1 0 1 3096.46 0.0551 0.0816 5 0 5

3096.54 0.0178 0.0835 3 2 1 3096.90 2 .6891 0.0802 7 1 6

3096.95 0.0041 0.0656 7 2 6

3097.22 0.0053 0,0955 2 1 2

3097.65 0,0047 0,0877 6 1 5

3097,76 0 .0044 0.0739 6 3 4

3098.81 0.0048 0.0951 3 2 2

3098.85 0.0785 0.0887 8 4 5

3099, 01 0.0022 0.0737 5 3 3

3099, 54 9.2244 0.0845 4 2 3

3099,76 5.8166 0.0942 4 0 4

1" E" L BAND

cm-1

11 4 8 1843 .02 5.243402 2NU2

4 4 1 488 . 10 0.001994 2NU2

7 3 5 816.72 3.273499 2NU2

4 0 4 222.06 2.831638 2NU2

6 5 2 888 .60 0.003511 2NU2

5 1 4 399.46 1.912338 2NU2

3 1 3 142.28 2. 156792 2NU2

8 2 6 982 ,91 3. 773034 2NU2

4 2 3 300.35 1.567300 2NU2

3 2 2 206 .30 1,297651 2NU2*

7 2 5 782 .40 1.512999 2NU2

5 1 4 399 .46 1,638916 2NU2

11 5 7 1985,83 0.365425 NUl

5 3 3 504.00 2.492169 2NU2*

7 2 5 782 ,40 3.983004 2NU2*

2 1 2 79 .48 1.500000 2NU2*

10 8 3 2254.34 0.051950 NU3

8 2 6 982.91 0.018354 2NU2

13 3 10 2414.73 0.074330 NU3

10 4 7 1581 .34 5.051335 2NU2

4 1 3 275.52 2.047924 2NU2*

6 3 4 648 .97 2.963539 2NU2

3 2 2 206.30 1.297651 2NU2**

4 3 2 382.52 1.848533 2NU2*

3 0 3 136.77 1.741385 2NU2*

9 4 5 2998 .78 7.39 NUl***

6 3 4 648.97 0.017960 2NU2

2 1 2 79.48 1.500000 2NU2**

3 3 1 285.23 0.004153 2NU2

8 4 5 1122.72 4.264036 2NU2*

2 2 1 134.91 0.833333 2NU2*

3 3 1 285.23 1 .035682 2NU2*

7 6 2 1216.20 0.004975 NUl

10 5 5 1724.72 0.005774 NU3

11 3 8 1813.26 5.642326 2NU2

4 1 3 275.52 2. 047924 2NU2**

3 2 2 206. 30 1.297651 2NU2

4 3 2 382.52 1. 848533 2NU2**

5 3 3 504.00 2.492169 2NU2

3 0 3 136.77 1.741385 2NU2**

9 4 6 1340.89 4.734521 2NU2

2 1 2 79,48 1.500000 2NU2

4 3 2 382,52 0.011053 2NU2

3 3 0 285 ,43 1.092505 2NU2*

7 2 5 782 ,40 3.983004 2NU2

8 5 3 1255,92 0. 018297 NUl

2 2 1 134.91 0.833333 2NU2**

6 2 4 602 .77 4.225862 2NU2*

6 4 3 756.75 2.878858 2NU2*

4 1 3 275.52 0.835095 2NU2*

9 3 6 1282 .92 1.416234 2NU2

5 4 2 610.12 2 .024051 2NU2*

4 3 2 382 ,52 1 .848533 2NU2

4 1 3 275,52 2.047924 2NU2

8
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

nm rm ~ 2 U 1 1 1 1 1 1 atm.

3100.33 0.0021 0.0705 4 3 1 3100.64 0.0029 0.0694 7 1 7

3101.16 29.7089 0.0994 2 1 2

3101.81 0.0020 0.0389 11 0 11

3101.90 0.5262 0.0705 8 3 6

3101.93 0.0033 0.0835 3 2 1 3102.18 0.0073 0.1032 2 0 2

3102.30 0.0066 0.0759 5 3 2

3102.36 0,0226 0.0996 0 0 0

3102.45 2.8045 0.0833 3 2 2

3103.02 14,3570 0.0955 2 1 2

3103.37 0.0307 0.0701 10 2 8

3103.44 0.0624 0.0975 3 0 3

3104.58 0.0012 0.0699 4 3 2

3104.94 0.0461 0.1111 1 1 0

3105.81 0.3969 0.0732 7 3 5

3106.02 0.0016 0.0801 6 3 3

3106.72 0,0013 0.0862 4 2 2

3106.73 0,0307 0.0912 5 1 4

3107. 32 8,8801 0.0835 3 2 1 3107.35 0.0184 0.0884 5 2 3

3107.60 0,0144 0.0957 2 1 1 3108.20 2,2180 0.0739 6 3 4

3108.42 0.0042 0.0996 0 0 0

3108.63 0.0016 0.0909 4 3 2

3108.89 0.0025 0.0627 5 3 2

3109.35 1.0823 0.0737 5 3 3

3109.65 0.0115 0.0975 3 0 3

3109.74 3 .1980 0.0699 4 3 2

3110.29 2 .3448 0.0877 6 1 5

3110.57 1 .0714 0.0705 4 3 1 3110.87 0.0598 0.0937 3 1 2

3110.93 0.0170 0.0934 4 1 3

3111.99 0.0040 0.0893 6 2 4

3112.08 3.5955 0.0862 4 2 2

3112.16 2 .3813 0.0951 3 2 2

3112.26 0.0194 0. 1044 2 1 1 3112.40 3 .3142 0.0759 5 3 2

3112.67 0.0050 0.0425 8 6 2

3112.73 0 .0034 0.0884 5 2 3

3112.83 0.0057 0.0912 5 1 4

3112.88 0.0165 0.0801 8 1 8

3113.03 0,0014 0.0504 10 5 6

3113.12 0.0139 0.0567 10 2 9

3113.29 0.0139 0. 1044 1 1 1 3113.36 0.0027 0.0957 2 1 1 3113.49 0.0060 0.0886 7 2 5 3113.57 0,0280 0.0482 9 0 9

3113.69 0,0011 0.0825 4 2 3

3114.47 11.3161 0.0996 0 0 0

3114,53 0.0293 0. 1021 2 0 2

3115.25 0.0018 0.0613 11 3 9

3115.87 31.2022 0.0975 3 0 3

3115.94 0.7877 0.0801 6 3 3

J" Kc E" L BAND

cm"i

4 0 488 . 13 1 .088294 2NU2*

8 4 4 1131 .76 0 . 006860 NUl

3 0 3 136.77 1. 741385 2NU2

12 2 10 1960 .22 0.025215 NU3

8 5 1122 .72 4. 264036 2NU2

3 3 0 285.43 1.092 505 2NU2**

1 1 1 1634.97 0.755253 2NU2***

5 1 610.35 2 .066632 2NU2*

1 1 1 37.13 1 . 000000 2NU2*

3 3 1 285.23 1 .035682 2NU2

2 2 1 134.91 0. 833333 2NU2

10 3 7 1538.23 5.910419 2NU2

3 1 2 173 .36 2.185861 2NU2*

1 488 . 10 1 . 082946 2NU2**

1 0 1 1618 .55 1 • 500000 2NU2***

7 4 927 . 77 3.63 7027 2NU2

6 4 2 757.78 3.075987 2NU2*

4 3 1 383.85 2.167225 2NU2**

5 2 3 446 . 50 4. 214107 2NU2*

3 3 0 285.43 1 .092505 2NU2

5 3 2 508 . 8 1 3.442901 2NU2*

2 2 0 136 .17 1.258755 2NU2*

6 4 3 756. 75 2.878858 2NU2

1 1 1 37.13 1 . 000000 2NU2**

5 2 3 2053.98 0.436045 2NU2***

5 ft 1 1045.07 0 . 00 T 286 NUl

5 4 2 610.12 2. 024051 2NU2

3 1 2 173.36 2. 185861 2NU2**

4 4 1 488 . 10 1 . 082946 2NU2

6 2 4 602 ,77 4, 225862 2NU2

4 4 0 488.13 1,088294 2NU2

3 2 1 212.15 2, 538253 2NU2*

4 2 2 315 .79 3.642913 2NU2*

6 3 3 661 . 56 4.829435 2NU2*

4 3 1 383.85 2 • 167225 2NU2

4 1 3 275.52 0. 835095 2NU2

2 0 2 1664.97 2.074578 2NU2***

5 4 1 610.35 2 . 066632 2NU2

9 8 1 2009 .87 0.032025 NU3

5 3 2 508 .81 3.442901 2NU2**

5 2 3 446 . 50 4.214107 2NU2*-*

7 2 5 782 .40 0.024347 2NU2

1

1

7 5 2 321,89 0. 107152 NU3

1

1

3 8 1813,26 0.316624 NU 1 2 0 2 70 , 08 0.755253 2NU2*

2 2

0' 136.17 1 .258755 2NU2**

7 3 4 842 .38 5.918411 2NU2*

10 3 8 1446 . 16 0. 106449 NUl

3 3 0 1907 .63 0. 131472 2NU2***

1 1 1 37.13 1 . 000000 2NU2

2 1 1 95.17 2.074578 2NU2*

1

2

4 8 2205.65 C- t~.\j ^ m \j ^ 0.720922 NUl

3 1 2 173.36 2.185861 2NU2

6 4 2 757.78 3.075987 2NU2

707-944 0 - 64 -2 9
LINE HALF

FREQUENCY STRENGTH WIDTH J' Ka Kc

cm ^ CIT1~1 cm ' am cm atm

3116.39 0 .3480 0.0783 9 2 7

3116.68 0.0111 0.0937 3 1 2

3116.70 0.4801 0.0925 5 3 3

3116.85 0.0032 0.0934 4 1 3

3117,10 0.0018 0.0578 5 4 1 3117.12 0.0017 0.0620 6 4 3

3118.12 9.1917 0o0884 5 2 3

3118.93 0.0186 0.0659 9 2 7

3118.94 15.3668 0.0912 5 1 4

3119.12 7.2213 0.0957 2 1 1 3119.65 0,0026 0. 1044 1 1 1 3120.18 0.0043 0.0569 10 5 5

3120.66 0,0054 0. 1021 2 0 2

3120.86 0.0826 0. 1075 1 0 1 3121.63 0.0354 0.0613 10 4 7

3121.66 1 .3799 0.0832 7 3 4

3121.76 0.0099 0.0511 9 1 9

3122.49 29.9070 0.0937 3 1 2

3122.78 8.5222 0.0934 4 1 3

3123.07 2.0057 0.0893 6 2 4

3123.13 0.3787 0.0840 8 2 6

3124.99 0.0385 0.0994 3 1 2

3125.12 2 .9878 0.0886 7 2 5 3126.01 0.0339 0.0639 9 4 6

3126.02 6.9402 0. 1044 1 1 1 3126.61 0.2500 0.0650 8 4 5

3126.78 0.3058 0. 0574 5 4 2 3126.80 14.6442 0.1021 2 0 2

3126.81 0.1711 0.0645 7 4 4

3126.85 0.9180 0.0578 5 4 1 3126.86 0.8358 0. 0620 6 4 3

3126.95 0.0153 0. 1075 1 0 1 3127.37 0.2793 0.0637 6 4 2

3127.75 0,0409 0.0994 3 0 3

3127.89 0.0054 0.0654 8 J 8

3128.49 0.5182 0.0680 7 4 3

3128.71 0.2265 0.0844 8 3 5 3129.36 0.0087 0.0949 2 2 1 3129.63 0 .0066 0. 0546 11 4 8

3129.94 0.0037 0.0812 10 5 6

3130.41 0 .0747 0.0715 8 4 4

3130.41 0.0061 0.0446 11 2 10

3131.33 0.1309 0.0554 8 0 8

3131.94 0.0232 0.0755 11 3 8

3132.49 0.0289 0.0806 10 3 7

3133.05 41,3221 0. 1075 1 0 1 3134. 32 0.2717 0.0835 9 3 6

3134. 54 0.0017 0.0681 6 2 4

3134.55 0.1083 0. 0740 9 4 5 3134.69 0.0388 0.0567 9 1 8

3135.09 0.0041 0.0659 8 1 7

3135.28 0.0133 0.0755 10 4 6

3136.07 0.0016 0. 0949 2 2 1 3136.31 0.0537 0.0894 7 4 4

J" Ka Kc E" L BAND

cm~^

9 3 6 1282.92 6.247031 2NU2

3 2 1 212.15 2. 538253 2NU2**

6 2 4 602.77 0.863547 2NU2

4 2 2 315.79 3.642913 2NU2**

5 5 0 742.10 1. 101100 2NU2*

6 5 2 888 .60 2 .085226 2NU2*

5 3 2 508.81 3.442901 2NU2

10 5 6 1718.77 0.266747 NUl

5 2 3 446.50 4.214107 2NU2

2 2 0 136.17 1.258755 2NU2

2 0 2 70.08 0.755253 2NU2**

11 7 4 2321 .94 0. 108914 NU3

2 1 1 95. 17 2.074578 2NU2**

1 1 0 42 .37 1. 500000 2NU2*

10 5 6 1718.77 5.482102 2NU2

7 4 3 931.22 4.268667 2NU2

10 2 8 1438 .00 0. 108277 NUl

3 2 1 212. i5 2.538253 2NU2

4 2 2 315.79 3.642913 2NU2

6 3 3 661.56 4.829435 2NU2

8 3 5 1050 . 15 6.368783 2NU2

3 0 3 1731.89 2.185861 2NU2***

7 3 4 842.38 5.918411 2NU2

9 5 5 1474.99 4. 736397 2NU2

2 0 2 70.08 0.755253 2NU2

8 5 4 1255.16 3.901175 2NU2

5 5 1 742.10 1. 100600 2NU2

2 1 1 95.17 2.074578 2NU2

7 5 3 1059.65 3.012848 2NU2

5 5 0 742. 10 1. 101100 2NU2

6 5 2 888.60 2.085226 2NU2

1 1 0 42 .37 1.500000 2NU2**

6 5 1 888 .63 2.089996 2NU2

2 1 2 1677.08 1.741385 2NU2^<-*-«-

9 4 5 1360.28 0.001245 NU3

7 5 2 1059.85 3.039271 2NU2

8 4 4 1131 .76 5.709388 2NU2

3 1 2 173.36 0.300506 2NU2*

12 6 7 2433.85 0.169033 NU3

11 4 7 1899.06 1.370216 2NU2

8 5 3 1255 .92 3.41 NU2-

12 4 9 2124.98 0.077267 NU3

8 5 3 1255.92 0.580 NU1 +

11 4 7 1899.06 8.484859 2NU2

10 4 6 1616.51 8. 179783 2NU2

1 1 0 42 .37 1. 500000 2NU2

9 4 5 1360.28 7. 165263 2NU2

7 6 1 1216.20 0.000189 NU3

9 5 4 1477.31 5.113359 2NU2

10 4 7 1581.34 0.284777 NUl

7 4 4 927.77 0.037317 2NU2

10 5 5 1724.72 6.465380 2NU2

3 1 2 173.36 0.300506 2NU2**

8 3 5 1050. 15 0.898681 2NU2

10
LINE HALF

FREQUENCY STRENGTH WIDTH J' K

cnn~^ cm"l

gm cm~2 atm.

3136.70 0,0200 0.0861 7 1 7

3137 . 00 0.0032 0, 0909 4 3 2

3139. 10 0 .0092 0,0 524 9 5 5

3139.53 0.0218 0,0687 6 2 5

3139. 95 0.0025 0,0398 7 6 1 3139.95 0.0076 0,0398 7 6 2

3 140 . 39 0 ,0057 0, 060

1

9 1 8

3140 . 44 0.0467 0. 1054 2 1 2

3142 . 2

1

0,0031 0,0548 9 5 4

3142 .79 4.3267 0 , 0949 2 2 1 3144 .15 0.0020 0, 0662 9 2 7

3 144 .15 0.0079 0, 0974 4 1 3

3145 .83 0.0056 0,0513 1

1

3 9

3146 .97 0.0137 0.0634 8 1 7

3147.84 0 .0035 0.0947 4 1 3

3147 .92 0.0122 0 ,0704 8 2 6

3149 .35 0 .0031 0,0489 1

1

1 10

3151 . 34 1.6066 0,0909 4 3 2

3152.00 0.0012 0, 0960 3 1 3

3152.20 0.0163 0,0961 4 0 4

3152.26 0,2055 0. 0477 6 5 2

3152.32 0.0556 0,0518 7 5 3

3152 . 37 0 .0685 0. 0478 6 5 1 3152.42 0 .1668 0.0521 7 5 2

3153 .45 0.0909 0.0545 8 5 4

3154.00 0.0135 0.0554 10 5 6

3154 . 32 0.0303 0.0556 8 5 3

3154. 73 0.0133 0.0558 9 5 5 3155 .04 0 .0028 0.0914 3 2 1 3155.32 0.2107 0. 0902 6 1 6

3155.59 0 . 040

1

0.0 583 9 5 4

3155.79 0.0205 0 . 1026 3 1 3

3156 . 47 0 .0046 0.0608 10 5 5

3156.63 0.0014 0.0814 5 3 2

3157.41 0 .0010 0.0829 3 3 0

3157.46 0 .0030 0 .0948 4 1 4

3157.71 0 ,0076 0.0421 10 1 10

3158.15 0,0107 0.0951 4 2 2

3158.86 0,03 74 0.0949 3 2 1 3159.18 0,0023 0.0886 5 2 3

3161.73 0,0012 0. 0941 2 2 0

3161 .98 0,0038 0.0574 10 4 7

3162 . 04 0,0229 0 .0440 10 0 10

3162.47 0 ,0092 0.0979 2 2 0

3163 . 09 0,0201 0, 0947 5 2 3

3163.82 0,5918 0,0960 3 1 3

3163.97 0,0052 0 ,0569 1

1

3 7 3164.12 0 ,0897 0,0780 6 3 3

3164.61 0,0292 0 , 0736 6 1 6

3164 .80 0 , 0026 0,0653 1

1

4 8

3165.32 0 ,0923 0,1111 1 1 0

3165.38 0,0085 0,0512 8 4

3165.70 0,0102 0,0689 9 4 5 3166.41 0,0257 0,0523 8 5 3

J" Kc E" L BAND

cm"'

6 2 4 602,77 0.035782 2NU2

5 2 3 446 . 50 0.436045 2NU2*

10 7 4 2054,40 0.078635 NU3

7 5 2 1059.85 0.011802 NUl

8 8 0 1789. 10 0.014826 NU3

8 8 1 1789. 10 0.014826 NU3

8 4 5 1122.72 0.045574 2NU2

1 0 1 1618. 55 1. 500000 2NU2***

10 7 3 2054.40 0.079027 NU3

3 1 2 173.36 0.300506 2NU2

8 5 4 1255. 16 0.030877 2NU2

4 0 4 1817.50 2.047924 2NU2***

12 5 8 2275.44 0. 143644 NU3

9 5 4 1477.31 0.005631 NU3

3 2 2 1813.81 0.835095 2NU2***

9 5 5 1474,99 0.157672 NUl

12 3 9 2105,90 0.080345 NU3

5 2 3 446,50 0.436045 2NU2

2 2 0 136, 17 0.101693 2NU2*

3 1 3 1739,51 2.831638 2NU2***

6 6 1 1045.07 1. 111607 2NU2

7 6 2 1216,20 2. 119434 2NU2

6 6 0 1045 .07 1. 111654 2NU2

7 6 1 1216.20 2. 119964 2NU2

8 6 3 1411,65 3.073714 2NU2

10 6 5 1875,00 4.913223 2NU2

8 6 2 1411 ,68 3.077042 2NU2

9 6 4 1631 ,27 4.001691 2NU2

4 1 4 224,83 0. 123609 2NU2*

5 2 3 446.50 0.057105 2NU2

9 6 3 1631 .41 4.017231 2NU2

2 0 2 1664,97 2. 156792 2NU2***

10 6 4 1875,53 4.974368 2NU2

6 2 5 552,92 0.312103 2NU2*

4 2 3 1907,99 0. 131472 2NU2***

3 2 1 212,15 0.123609 2NU2*

11 3 9 1695,03 0.027489 NU3

4 1 3 1875,49 3. 642913 2NU2***

3 1 2 1772,41 2.538253 2NU2***

4 3 2 2004,81 0.436045 2NU2***

3 1 3 142,28 0. 101693 2NU2^^

1

1

6 6 2142 ,69 0, 142262 NU3

11 2 9 1690,70 0,027627 NU3

2 1 1 1693,65 1,258755 2NU2***

5 1 4 2000,90 4,214107 2NU2***

2 2 0

' 136,17 0, 101693 2NU2

12 6 6 2437,56 4,215931 NUl

7 2 6 709.60 0,271048 2NU2

7 4 3 931 ,22 0,008274 NUl

12 5 7 2300.80 2, 124861 NUl

1 0 1 23.79 1, 500000 2NU2*

9 7 3 1810.63 0,053898 NU3

10 3 8 1446 .16 0,409296 2NU2

9 7 2 1810.63 0,053971 NU3

11
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq K, cm * gm cm 2

~ 1 \^\\\ nU +m1 1 1 1. 3166.71 0.2166 0.0929 5 1 5

3167.26 0.0795 0.0737 7 3 4

3167.92 1 .3868 0.0914 3 2 1 3169.24 0.0133 0.0914 5 1 4

3169.29 0.2054 0.0872 4 2 2

3169.49 0.0034 0.0813 9 5 5 3169.58 1 .4784 0.0948 4 1 4

3169.83 0,6794 0.0814 5 3 2

3170.06 0.0162 0.0720 8 4 4

3170.23 0.0536 0.0976 4 1 4

3170.92 0.0520 0.0740 7 2 5 3170.98 0.0283 0.0559 8 0 8

3171.72 0.0171 0.1111 1 1 0

3172.48 0.0388 0. 1044 2 1 1 3172.57 0.0145 0.1032 2 0 2

3173.08 0.2821 0.0876 6 4 3

3174.63 0.0451 0.0880 5 0 5

3174.91 0.5760 0.0941 2 2 0

3175.05 0.0219 0.0481 10 6 5

3175.24 0.0073 0.0470 10 t> 4

3175.38 0.0033 0.0920 6 2 4

3175.56 0.0089 0.0403 9 7 3

3175.56 0.0266 0.0403 9 7 2

3176.22 0.0082 0.0700 5 2 4

3177.08 0.0285 0.0675 10 3 8

3178. 13 46.13 36 0.1111 1 1 0

3178.70 0.0027 0.1032 2 0 2 3178.84 0.0218 0.0641 9 2 8

3178.84 0.0072 0. 1044 2 1 1 3179.69 0.2115 0.0812 5 2 3

3179.95 0.0130 0.0467 9 6 3

3180.09 0 .0066 0.0687 8 3 5

3180.60 0.0042 0.0475 10 6 5

3180.70 0.0014 0.0484 10 6 4

3181.37 0.0043 0.0463 9 6 4

3182.01 0.0130 0.0918 5 1 4

3182.22 0.1178 0.0741 7 4 3

3182.48 0.3777 0.0829 4 3 1 3182.96 0.0413 0.0640 8 1 7

3183.21 0.0232 0.0996 1 1 1 3183.30 0.0105 0.0340 8 8 0

3183.30 0.0314 0.0340 8 8 1 3183.64 0.0122 0.0409 7 6 2

3183.64 0.0247 0.0440 8 6 3

3183.64 0.0365 0.0409 7 6 1 3184.51 0.0111 0.0499 10 2 9

3184.64 0.0078 0.0441 8 6 2

3184.69 0.3855 0.0884 3 3 1 3184.84 7.2584 0. 1032 2 0 2

3185.10 0.1125 0.0601 8 1 8

3185.21 19.4248 0. 1044 2 1 1 3185.30 0.0769 0.0994 3 1 2

3185.49 0.0022 0.0825 4 2 3

3186.41 0.0020 0.0829 3 3 0

J

1/Kq Kc E

1L cm-1

4 2 2 315.79 0.091324 2NU2

8 2* 7 885.62 0.192937 2NU2

4 1 4 224 .83 0 . 123609 2NU2

5 0 5 1920.76 1.912338 2NU2***

5 1 5 326.64 0.091324 2NU2

1

0

4 6 1616.51 0. 959644 2NU2

3 2 1 212.15 0. 123609 2NU 2

6 2 5 552.92 0.312103 2NU2

9 3 7 1216.27 0.616 NU2 +

3 0 3 1731.89 3 . 004990 2NU2***

8 5 4 1255.16 0.074366 NUl

9 3 7 1216.27 0.10 NUl1 0 1 23.79 1 . 500000 2NU2**

2 0 2 70.08 2 . 074578 2NU2*

1 1 1 37.13 0.755253 2NU2*

7 3 4 842 ,38 0. 550367 2NU2

4 1 4 1821 ,61 3.911752 2NU2***

3 1 3 142 , 28 0 . 101693 2NU2

1 1 7 4 2321 ,94 5.877228 NU

1

1 1

-77 5 2321,89 5.881509 NU 1 6 1 5 2 146 . 28 4. 225862 2NU2***

10 8 2 2254. 34 7. 138077 NUl

1 0 8 3 2254.34 7.138103 NUl

6 5 1 888.63 0.005627 NU 1

1 1 4 7 1899 . 06 0.954846 NUl

1 0 1 23.79 1 . 500000 2NU2

1 1 1 37.13 0.75 5253 2NU2*'*^

1 0 3 7 1538.23 0. 380414 NUl

2 0 2 70 .08 2 .074578 2NU2''^*

6 1 6 447 ,24 0.057105 2NU 2

9 7 2 1810.63 3.116419 2NU2

9 2 0 lOoO . 38 0. 126905 2NU2

1

0

7 4 2054.40 4.05 8996 2NU2

1 0 7 3 2054.40 4.061130 2NU2

9 7 3 1810.63 3. 116005 2NU2

4 2 3 1907.99 1 .638916 2NU2***

8 3 6 1006 . 12 0. 519243 2 NU2

5 2 4 416.22 0.261722 2NU2

9 4 6 1 340 .89 0.269351 NU 1 0 0 0 0 .00 1 . 000000 2NU2*

9 9 1 2225.56 8 . 4037 19 Mill NU 1 9 9 0 2 225.56 8 . 40 37 19 NUl

7 7 1 1394.86 1 . 1 19792 2NU2

8 7 2 1590.74 2.03 NU2-

7 7 0 1 394 . 86 1.119797 2NU2

1

1

4 8 1843 . 02 0. 082847 Ml 1 0 NU3

8 7 1 1 590 . 74 1.93 NU2-

4 2 2 3 1 5 . 79 0. 161593 2NU2

1 1 1 37.13 0.755253 2NU2

9 2 7 1201 .95 0. 122288 NU 1 2 0 2 70 . 08 2 .074578 2NU2

3 0 3 136.77 2. 185861 2NU2*

3 3 0 285.43 0. 131472 2NU2*

4 2 3 300.35 0. 131472 2NU2*
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq K

cm1 n rn ^rn ~ 2 U M 1 1

1

otm.

3187.31 0.0075 0.0939 3 2 2

3187.54 0.0167 0.0613 11 5 6

3188. 16 0.0107 0.0951 3 1 2

3188.30 0.0031 0.0685 5 1 5

3188.98 0.0009 0.0633 10 5 5 3189.66 0.0043 0.0996 1 1 1 3189.90 0.0179 0.0748 6 2 4

3190.09 0.0093 0.0566 10 3 8

3190.86 0.0225 0.0571 10 5 6

3191 .58 0.0142 0.0994 3 1 2

3191.93 0.0458 0.0489 7 5 3

3192.06 0.0359 0.0589 9 4 6

3192. 17 0.0153 0.0493 7 5 2

3193.04 0.0101 0.0676 7 1 6

3193.94 0.0020 0.0951 3 1 2

3194.24 0.0036 0.0678 11 4 7

3195.08 0.0115 0.0760 6 0 6

3195.46 0.0042 0.0848 7 2 5

3196.10 11.6127 0.0996 1 1 1 3196.63 1.0993 0.0825 4 2 3

3197.34 0.0819 0.0994 3 0 3

3197.87 38.4548 0.0994 3 1 2

3198.15 0.0221 0.0747 6 2 4

3199.28 0.0844 0.0743 6 4 2

3199.71 0.0181 0.0896 4 2 3

3199.73 5.3386 0.0951 3 1 2

3200.27 1 .0215 0.0829 3 3 0

3200.36 0.0049 0.0765 10 2 9

3200.81 0.0350 0.0779 6 1 6

3200.94 0.0046 0.0633 9 3 6

3201.03 0.0088 0.0696 7 0 7

3201.18 0.0933 0. 1054 2 1 2

3201.64 0.0018 0.0638 8 3 5

3201 .84 0.0226 0.0473 9 6 4

3201 .96 0.0679 0.0475 9 6 3

3203. 17 0.0364 0.0378 8 7 1 3203. 17 0.1092 0.0378 8 7 2

3203. 54 0.0152 0.0994 3 0 3

3204. 12 0.0158 0.0974 4 1 3

3204.82 0.0260 0.0794 8 5 4

3205.66 0.0093 0.0641 9 5 4

3206.01 0.0749 0.0949 3 2 1 3207.20 0.0402 0.0733 5 2 3

3207.26 0.0215 0.0951 4 2 2

3207.32 0.1295 0.0840 5 4 2

3207.61 0.0015 0.0509 10 2 9

3207.66 0.0173 0. 1054 2 1 2

3208.54 0.0183 0.0979 2 2 0

3208.78 0.0513 0.0671 10 4 7

3209.23 0.0149 0.0690 4 2 3

3209.25 0.0117 0.0603 10 5 5 3209.75 40 .9463 0.0994 3 0 3

3210.31 0.0029 0.0974 4 1 3

3210.70 0.4528 0.0864 4 2 2

1" F" L BAND

cm-'

3 1 3 1739.51 1.297651 2NU2***

1

2

6 7 2433 .85 4. 458582 NUl

2 2 1 134.91 0. 300506 2NU2*

6 5 2 888 . 60 0. 000066 NU3

1

1

4 8 1843.02 0.753106 2NU2

0 0 0 0.00 1 . 000000 2NU2**

7 5 3 1059 .65 0.028700 NUl

1

1

5 7 1985 .83 0. 140157 NU3

1

1

6 5 2144. 12 3. 00 NU 1-

3 0 3 136.77 2. 185861 2NU2**

8 7 2 1590.74 0.032804 NU3

1 0 6 5 1875 . 00 0.112325 NU3

8 7 1 1590 .74 0.032814 NU3

QO 5 3 1255.92 0.004077 Ml 1 O

2 2 1 134 .91 0 . 300506

1

2

6 6 2437.56 0.265013 NU3

5 1 5 1922 .86 4 . 95 8 549 2 NU 2***

7 1 6 2309.74 3. 983004 2NU2***

0 0 0 0 .00 1 . 000000 2NU2

3 3 0 285.43 0 . 131472 2NU2

2 1 2 79.48 1 . 741385 2NU2*

3 0 3 136.77 2.185861 2NU2

{ 1 7 586.48 0.035782

1 3 5 0 1 6 . 72 0.431025 0 M 1 IT 2NU2

4 1 4 1821 .61 1 . 567300 2NU2''^*'*

2 2 1 134.91 0.300506 2NU2

4 2 3 300.35 0. 131472 2NU2

9 3 6 1282.92 0.084934 2NU2

5 0 5 1920.76 4.979001 2NU2***

10 2 9 1293 .66 0 . 084934 2NU2

8 4 4 1131 .76 0.00 1880 NU3

1 0 1 23.79 1 . 500000 2NU2*

8 7 2 1590*74 0.001180 NU3 + 10 7 3 2054.40 6.018378 NU 1

1 0 7 4 2054.40 6. 019433 NUl

9 8 2 2009 . 87 7.261219 NUl

9 8 1 2009.87 7.261215 NUl

2 1 2 79.48 1.741385 2NU2**

4 0 4 222.06 2 . 047924 2NU2*

9 4 5 1 360 .28 0. 669979 2NU2

10 4 7 158 1 . 34 0.720783 2NU2

3 1 2 173.36 2.538253 2NU2*

6 5 2 888.60 0. 009072 Mill NUl

4 1 3 275.52 3. 642913 2NU2*

6 3 3 661.56 0.303663 2NU2

1 0 5 6 1718 . 77 0.021485 NU 1

1 0 1 23.79 1 . 500000 2NU2**

2 1 1 95.1/ 1.258755 2NU2*

1

1

5 6 1999 . 02 2. 723522 (villi NUl

5 5 0 742 .10 0.001619 NUl

1

1

6 6 2142.69 4.667626 NUl

2 1 2 79.48 1 . 741385 2NU2

4 0 4 222 .06 2 .047924 2NU2**

3 3 1 285.23 0.161593 2NU2

13
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm ~ ^ ym cm 0 tm. 3211. 19 0.0145 0.0684 10 4 6

3211.48 0,0134 0,0677 9 4 5

3212.70 0.0139 0,0949 3 2 1 3213. 17 0,0056 0,0631 11 2 9

3213.83 0,0040 0.0951 4 2 2

3213.93 0.0229 0,0631 7 0 7

3214. lA 46 .6563 0,1054 2 1 2

3214.66 0,4485 0,0826 5 2 4

3214.68 0,0402 0.0947 5 2 3

3214,73 0,0433 0. 1021 2 2 1 3215.23 0,0874 0.0482 9 1 9

3215.28 0,0034 0.0979 2 2 0

3215.41 0,0040 0.0815 5 2 4

3215 . 54 0.0017 0.0831 6 2 5

3215.75 0,0040 0.0843 6 1 5

3216.51 7,8852 0.0974 4 1 3

3216.88 0.0410 0. 1026 3 1 3

3217. 10 0.0077 0. 0642 7 1 7

3218.02 0,0078 0.0798 9 2 8

3218.67 0,0189 0.0456 6 5 2

3218.72 0.0567 0.0457 6 5 1 3218.87 0.0010 0.0539 9 1 9

3219.39 37.4362 0.0949 3 2 1 3219.68 0,0214 0.0776 5 1 5

3219.98 0,3804 0.0727 5 4 1 3220.22 0,0430 0.0601 8 4 5 3220.40 0,0327 0.0961 4 0 4

3220.41 10.7494 0.0951 4 2 2

3220.80 0.0042 0.0927 7 3 4

3221.07 0,0074 0.0947 5 2 3

3221.15 0,0123 0.0949 2 2 0

3222.02 9,1560 0.0979 2 2 0

3223.26 0,0395 0.0952 2 2 1 3223.34 0,0207 0.0679 7 2 5 3223.37 0,0309 0.0511 9 0 9

3223.39 0,0076 0.1026 3 1 3

3224.48 0,0061 0.0703 4 2 2

3225.07 0,0028 0.0925 6 3 3

3225. 11 0,0086 0.0646 8 5 3

3225.72 0.3078 0.0711 7 1 6

3226. 13 0,3109 0.0650 7 0 7

3226.44 0,0013 0.0947 4 1 3

3226.70 0,0060 0.0961 4 0 4

3227.34 0,8624 0.0831 6 2 5

3227,47 20.1179 0.0947 5 2 3

3227.77 0,0266 0.0914 5 1 4

3228,89 0.2794 0.0454 8 6 3

3228.94 0.0931 0.0454 8 6 2

3229.01 0.0035 0.0671 7 1 6

3229. 33 0,1006 0.0819 8 2 7

3229.36 0.0C66 0.0920 6 2 4

3229,91 20,4780 0. 1026 3 1 3

3230. 16 0,0987 0.0616 9 3 7

3230.41 0.1647 0.0659 8 4 4

ill J Kc

II E L BAND

cm-1

11 6 5 2144,12 0. 181046 NU3

10 6 4 1875,53 0. 124623 NU3

3 1 2 173,36 2.538253 2NU2**

12 4 8 2205,65 0. 209597 NU3

4 1 3 275,52 3. 642913 2NU2**

6 1 6 2042 ,77 5 .983681 2NU2***

1 0 1 23 ,79 1.500000 2NU2

4 3 1 383 . 85 0.261722 2NU2

5 1 4 399 .46 4.214107 2NU2*

1 1 0 1640.51 1.500000 2NU2***

10 3 8 1446 . 16 0.030178 NU3

2 1 1 95.17 1.258755 2NU2**

5 1 5 1922 .86 1.711792 2NU2***

5 3 2 508.81 0.312103 2NU2*

5 2 4 2024,17 2.671788 2NU2***

4 0 4 222 , 06 2 . 047924 2NU2

2 0 2 70.08 2. 156792 2NU2*

6 0 6 2041 .76 5. 990506 2NU2***

8 3 5 1050 .15 0. 126905 2NU2

7 7 1 1394.86 0.014987 NU3

7 7 0 1394.86 0.014988 NU3

9 4 6 1340.89 0. 006488 NUl

3 1 2 173.36 2.538253 2NU2

6 4 2 757 .78 0.007497 NUl

6 3 4 648 .97 0.278030 2NU2

9 6 4 1631 .27 0. 1 10400 NU3 +

3 1 3 142 .28 2 .831638 2NU2*

4 1 3 275.52 3. 642913 2NU2

7 2 5 2392 . 58 5. 918411 2NU2***

5 1 4 399.46 4.214107 2NU2**

1 1 1 1634.97 1 . 244747 2NU2***

2 1 1 95.17 1 .258755 2NU2

2 1 2 79 .48 0.833333 2NU2*

8 1 8 744. 16 0.024347 2NU2

10 2 8 1438.00 0.030629 NU3

2 0 2 70.08 2. 156792 2NU2**

5 5 1 742 , 10 0.001985 NUl

6 2 4 2211.21 4. 829435 2NU2***

9 4 6 1340 .89 0. 597432 2NU2

8 4 5 1122.72 0.222677 NUl

8 3 6 1006 , 12 0.125531 NUl

3 2 2 206,30 0,835095 2NU2**

3 1 3 142 ,28 2,831638 2NU2**

5 3 2 508 ,81 0,312103 2NU2

5 1 4 399,46 4,214107 2NU2

5 0 5 325,35 1,912338 2NU2*

9 7 2 1810.63 6, 141896 NUl

9 7 3 1810.63 6, 142105 NUl

7 0 7 2180.65 1 ,838288 2NU2***-

7 3 4 842 .38 0,192937 2NU2

6 1 5 542 .91 4.225862 2NU2*

2 0 2 70,08 2. 156792 2NU2

10 5 6 1718.77 0.128613 NU3

9 6 3 1631 .41 0. 140500 NU3 +

14
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq K,

t#f n * ^ Pin ~" 1 gm cm~2Li 11 otm.

3230.86 0.1217 0.0356 7 7 1 3230.86 0.3650 0.0356 7 7 0

3230.93 0.0409 0.0717 6 1 5

3231.34 0.1191 0.0690 5 3 3

3231.87 0.0045 0.0520 8 0 8

3231.89 0.1073 0.0976 4 1 4

3232.06 0.0150 0.0939 3 2 2

3232.27 3.4961 0.0947 4 1 3

3232.52 0.0132 0.0909 5 3 2

3232. 59 0.1165 0.0830 7 2 6

3232. 76 0.0489 0.0569 9 5 5 3233.00 16.3336 0.0961 4 0 4

3233.39 0.0516 0.0729 9 3 7

3233.46 0,0135 0.0523 8 1 8

3233.50 0.0021 0.0859 7 2 5

3233.61 0,0068 0.0710 6 2 5 3233.75 0,0046 0.0886 5 2 3

3233.77 0,1475 0.0583 9 5 4

3233.93 0 .0049 0,0914 5 1 4

3234.65 0.3668 0,0761 5 3 2

3235.54 0.0012 0,0920 6 2 4

3235.98 0.0014 0,0661 10 6 5

3236.40 0.1308 0,0560 9 2 8

3236.67 19.7590 0.0952 2 2 1 3237.72 0.0139 0.0706 8 5 4

3237.94 0.3310 0.0787 4 4 1 3238.42 0.0198 0.0976 4 1 4

3238.73 0.00 2 8 0.0939 3 2 2

3240.09 13.2755 0.0914 5 1 4

3240.36 0.0053 0.0684 4 3 1 3241.39 0.0902 0.0880 5 0 5

3241 .72 3.2965 0.0920 6 2 4

3242.08 0.0016 0.0551 9 2 8

3242.76 0.1104 0.0708 4 4 0

3242.86 0.0055 0.0721 11 3 8

3243.02 0,3081 0.0712 8 2 7

3243.99 0.0362 0.0896 4 2 3

3244, 41 2.2776 0.0886 5 2 3

3244. 96 53.6439 0.0976 4 1 4

3245.40 7.5139 0.0939 3 2 2

3245.90 0.0552 0.0644 7 5 2

3246.06 0.0136 0.0854 3 3 0

3246.68 0.0748 0.0677 9 4 6

3247.31 0,1972 0.0596 7 4 4

3247. 37 0.0310 0.0900 5 1 5 3247.77 0.0167 0.0880 5 0 5

3247.83 0.0016 0.0596 6 3 4

3248.36 0.0087 0.0734 7 1 6

3248.90 0.0070 0.0436 9 0 9

3248.91 0 ,0299 0.0955 4 2 3

3249. 15 0,0144 0.0673 11 4 7

3249.49 0 ,1344 0.0690 7 1 7

3249.72 0 ,0023 0.0437 9 1 9

3250.61 0.0067 0.0896 4 2 3

J" E" L BAND

cm-1

8 8 0 1789 . 10 7.402783 NUl

8 8 1 1789. 10 7.402783 NUl

7 5 2 1059.85 0. 002023 NU3

4 4 0 488 . 13 0. 116422 2NU2

7 1 7 2181.12 6. 998008 2NU2***

3 0 3 136.77 3 . 004990 2NU2-**-

3 1 3 142 .28 1.297651 2NU2*

3 2 2 206.30 0.835095 2NU2

5 2 3 2053.98 3 . 44290

1

2NU2***

6 3 3 661 .56 0.271048 2NU2

10 6 4 1875.53 4. 830967 NU 1 3 1 3 142.28 2.831638 2NU2

1 0 4 6 1616.51 1.314980 NU 1 7 0 7 2180.65 7. 000291 ^ K \ V 1 \t \J \J 2NU2***

6 3 4 2271.70 1 . 512999 2NU2***

6 1 6 2042 .77 1.783035 2NU2***

4 3 2 382.52 0.436045 2NU2*

10 6 5 1875.00 4.857731 NUl

5 0 5 325 .35 1.912338 2NU2**

4 4 1 488 . 10 0. 119405 2NU2

6 1 5 542 .91 4.225862 2NU2**

1

1

5 6 1999 . 02 0 . 799607 2NU2

1 0 4 7 1581.34 0.087251 NU3

2 1 2 79 .48 0.833333 2NU2

7 4 3 2572.13 9.52 NUl***

5 3 2 508 .81 0. 119405 2NU2

3 0 3 136,77 3 . 004990 2NU2**

3 1 3 142 .28 1 .297651 2NU2**

5 0 5 325.35 1 .912338 2NU2

4 2 2 1922 .92 2.167225 2NU2***

4 1 4 224.83 3.911752 2NU2*

6 1 5 542 .91 4. 225862 2NU2

9 5 5 1474.99 0.019752 NUl

5 3 3 504.00 0. 116422 2NU 2

12 5 7 2300.80 0.411017 NU3

9 3 6 1282 .92 0.493418 NUl

4 1 4 224.83 1.567300 2NU2*

4 3 2 382.52 0.436045 2NU2

3 0 3 136.77 3 . 004990 2NU2

3 1 3 142.28 1 .297651 2NU2

8 4 5 1122 .72 0.427306 2NU2

3 2 1 1819. 34 1 . 092505 2NU2***

10 5 5 1724.72 3. 272354 NU 1 6 6 3 1411.65 0.056441 NU3

4 0 4 222 • 06 3.972803 2NU2*

4 ] 4 , 224,83 3.911752 2NU2**

6 6 1 1045 , 07 0. 000772 NU 1 6 2 5 2161 . 30 3.799063 2NU2***

8 1 8 2337,70 8.007087 2NU2***

3 1 2 1772.41 1.970843 2NU2***

1 2 5 8 2275 .44 3, 784189 NUl

8 2 6 982 .91 0, 143980 NUl

8 0 8 2337.53 8,007851 2NU2***

4 1 4 224.83 1 , 567300 2NU2**

15
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm ' gm cm -2

cm 1 otm.

3251.30 0 .0084 0. 0848 7 2 5

3251 .47 0.0666 0.0628 7 4 3

3251.49 0.0044 0.0830 3 3 1 3252.43 0.0017 0.0422 7 6 1 3253.07 0.0022 0.0604 8 2 6

3253.25 0,0260 0.0918 5 1 4

3254. 15 45,0823 0.0880 5 0 5

3254.60 0,4662 0.0713 6 3 4

3254.62 0.0148 0.0829 4 3 2

3254.63 0.0012 0.0601 7 2 6

3256.01 0.2793 0,0422 7 6 2

3256.01 0,8380 0.0422 7 6 1 3257.23 18.0800 0.0896 4 2 3

3257.29 0.0016 0.0848 7 2 5

3258.02 0.4997 0.0557 8 5 4

3258.12 0. 1760 0.0566 8 5 3

3258,72 0.0079 0.0815 5 2 4

3259. 17 0.0048 0.0918 5 1 4

3260.22 0.0866 0.1021 2 2 1 3260,42 0.0037 0.0803 5 3 3

3260.44 15.5056 0. 0900 5 1 5

3260. 50 0.0230 0,0760 6 0 6

3261.31 0.0098 0,0724 5 1 4

3262.02 0.0264 0,0909 5 3 2

3262. 50 0.1820 0,0774 6 1 5 3262.78 0.0074 0.0927 5 2 4

3263.28 4. 1894 0.0848 7 2 5 3263.37 0.0699 0.0779 6 1 6

3263.60 0. 1704 0.0809 6 3 3

3263.79 0 .0016 0.0927 7 3 4

3263 .99 O.OOlO 0.0925 6 3 3

3264. 12 0.0233 0. 0701 10 4 6

3264,27 0.0870 0.0740 6 0 6

3264. 33 0.0100 0.0589 8 1 8

3265.09 12 .9917 0.0918 5 1 4

3266.04 0.0937 0.0662 8 3 6

3266. 1

1

0.0858 0.0704 6 5 -2

3266.35 2,3549 0.0806 6 1 5 3266.58 0,0246 0.0949 2 2 0

3266.96 0,0043 0.0760 6 0 6

3267.00 0,0160 0, 1021 2 2 1 3267.21 0.0858 0,0795 4 1 4

3267.28 0.0013 0,0620 9 6 4

3268.36 0.0067 0,0751 6 3 4

3268.62 0,0107 0.0884 4 3 1 3268.88 0 ,0037 0.0673 7 3 4

3269. 13 0,0049 0.0909 5 3 2

3269.67 0,0288 0.0626 6 5 1 3269,92 0,0129 0.0779 6 1 6

3269,94 0,0017 0.0893 6 2 4

3270.48 4.2197 0.0927 7 3 4

3270.78 0.0112 0.0591 8 2 7

3270.95 2.8182 0.0925 6 3 3

3271.40 0.0023 0.0497 10 0 10

J" Kc E" L BAND

cm"i

7 1 6 704.22 3.983004 2NU2*

8 6 2 1411.68 0.057059 NU3

3 2 2 1813.81 1.035682 2NU2***

8 7 2 1590.74 6.263444 NUl*

9 1 9 920.21 0.018354 2NU2

4 2 3 300.35 1.638916 2NU2*

4 1 4 224.83 3.911752 2NU2

5 4 1 610.35 0.278030 2NU2

4 2 3 1907.99 1.848533 2NU2***

7 1 7 2181.12 1.816721 2NU2***

8 7 1 1590.74 6.263414 NUl

8 7 2 1590.74 6.263444 NUl

4 1 4 224.83 1.567300 2NU2

7 1 6 704. 22 3.983004 2NU2**

9 6 3 1631.41 4. 505 NUl9 6 4 1631.27 4. 76 NUl5 1 5 326.64 1.711792 2NU2*

4 2 3 300 .35 1,638916 2NU2**

1 1 0 42.37 1, 500000 2NU2*

5 2 4 2024. 17 2,492169 2NU2***

4 0 4 222.06 3.972803 2NU2

5 1 5 326,64 4.958549 2NU2*

6 5 1 888,63 0.000613 NU3

5 2 3 446,50 3.442901 2NU2*

7 4 4 927.77 0, 147419 NUl

4 1 3 1875.49 2,444582 2NU2***

7 1 6 704.22 3, 983004 2NU2

5 0 5 325.35 4,979001 2NU2*

5 4 2 610.12 0,303663 2NU2

7 2 5 782 .40 5,918411 2NU2**

6 2 4 602.77 4,829435 2NU2**

11 5 7 1985.83 3,652101 NUl

7 4 3 931.22 0.002241 NU3

8 4 5 1122.72 0.007182 NUl

4 2 3 300.35 1.638916 2NU2

9 5 5 1474.99 0. 109168 NU3

7 4 3 931.22 0.253734 2NU2

6 0 6 446.71 1.852055 2NU2

1 1 1 37.13 1,244747 2NU2*

5 1 5 326.64 4.958549 2NU2**

1 1 0 42 ,37 1.500000 2NU2**

5 4 1 610.35 0.004729 NUl

10 5 5 1724.72 0.586260 2NU2

6 2 5 2161.30 2,963539 2NU2***

4 2 2 315.79 2, 167225 2NU2*

7 6 1 1216,20 0.004214 NUl

5 2 3 446 . 50 3.442901 2NU2**

7 4 4 927,77 0.250934 2NU2

5 0 5 325,35 4.979001 2NU2**

5 3 3 504,00 0.863547 2NU2*

7 2 5 782 ,40 5.918411 2NU2

8 5 4 1255.16 0.015469 NUl

6 2 4 602 .77 4.829435 2NU2

10 4 7 1581.34 0.001525 NU3

16
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

c rm ~" 1 LlTl ' cm ~

gm cm-2 aim.

3271.87 3.9743 0.0815 5 2

3271.95 0.1032 0.0558 8 1 3272.03 0.0855 0.0704 10 2

3272.49 0.0775 0.0880 4 3

3272.76 0.0206 0.0865 5 3

3273.07 0.0020 0.0587 7 1 3273.36 0.0861 0.0590 6 4

3273.42 11.5179 0.0760 6 0

3273.78 43.3084 0.1021 2 2

3273.89 0.1059 0.0573 6 4

3274.25 0.0271 0.0854 3 3

3274.60 0.0736 0.0752 10 3

3275. 16 0,3186 0.0589 6 4

3275.48 0.0154 0.0873 6 2

3275.76 0.0020 0.0884 4 3

3275.80 0,1160 0.0740 7 3

3275.87 0.0137 0.0710 6 2

3276.25 13.1878 0.0909 5 3

3276.47 34.9525 0.0779 6 1 3276.81 0.0072 0.0628 9 0

3276.99 0.0015 0.0769 8 3

3277.40 0.0016 0.0503 8 2

3277.56 0.5567 0.0398 8 3

3277.58 0.2703 0.0711 9 4

3277.60 0 .0016 0.0685 8 3

3278.32 0.0459 0.0631 7 0

3278.42 0.016 3 0.0892 3 3

3278.47 0.0011 0.0682 7 3

3278.53 0.0011 0.0759 8 2

3278.58 0.2815 0.0735 6 0

3278.69 0.0342 0.0845 6 3

3278.79 0.0692 0.0648 9 1 3278.87 0.0248 0,0984 3 2

3279.07 0.8791 0,0676 8 4

3279.22 0.0017 0.0613 8 1 3279,41 0.0015 0.0388 6 6

3279.41 0.0046 0.0388 6 6

3279.64 0.0154 0,0642 7 1 3280.06 12.3204 0.0949 2 2

3280. 14 0.0034 0.0539 7 5

3280.47 0.0070 0.0671 7 1 3280.63 0.8282 0.0893 6 2

3280.72 0.0011 0.0834 9 3

3281.36 0.0050 0.0854 3 3

3282.39 0.0025 0.0710 6 2

3282.91 5.3299 0.0884 4 3

3283.01 0.7731 0,0388 6 6

3283.01 2,3193 0.0388 6 6

3283.52 0,0296 0.0829 4 3

3283.74 0.7692 0.0769 8 3

3284.10 0.5684 0.0537 7 5

3284.15 1.7058 0.0539 7 5 3284.69 0.0080 0, 0843 6 1 3284.75 0.0020 0,0543 9 2

J" Kc E" L BAND

cm~'

4 5 1 5 326 .64 1 . 71 1792 2NU2

8 9 7 1216.27 0. 033194 NU3

8 1

1

4 7 1899 . 06 0.260837 NU3

2 5 0 5 325 .35 0.011053 2NU2

3 6 0 6 446 .71 0. 016149 2NU2

7 7 5 2 1059.85 0. 000093 NU3

3 5 5 0 742 .10 0 .098702 2NU2

6 5 1 5 326 . 64 4. 958549 2 NU2

1 1 1 0 42 . 37 1 . 500000 2NU2

3 7 6 2 1216.20 0.033870 NU3

0 3 2 1 212.15 1 .092505 2NU2*

7 1

1

5 6 1999 . 02 0.359370 NU3

2 7 6 1 1216.20 0.033963 NU3

5 5 1 4 2000.90 3 . 129447 2NU2***

1 4 2 2 315.79 2 . 167225 2NU2**

5 6 4 2 757.78 0.431025 2NU2

5 6 1 6 447 .24 1.783035 2NU2*

2 5 2 3 446 • 50 3 . 442901 2NU2

6 5 0 5 32 5.35 4. 979001 2NU2

9 9 3 6 1282.92 0.01 1425 NUl

6 9 4 5 1360.28 1 . 797448 NU 1*

7 8 1 8 2337.70 1.833129 2NU2***

5 8 2 6 982,91 6.368783 2NU2

5 1 0 5 6 1718.77 3 . 697402 NUl

5 8 6 2 1411.68 0.014126 NU 1 7 6 1 6 447 .24 5.983681 2NU2*

1 4 0 4 222 . 06 0.004153 2NU2

5 7 2 6 2318. 53 3. 273499 2NU2***

6 8 1 7 882 .93 3. 773034 2NU2*

6 7 3 5 816.72 0. 130226 NUl

4 7 0 7 586.26 0. 01 7960 2NU2

8 10 3 7 1538.23 0.110021 NU3

2 2 1 1 95.17 1 . 666667 2NU2*

5 9 5 4 1477. 31 3. 682999 NUl

7 7 2 6 2318.53 4.913532 2NU2***

0 7 7 1 1394.86 6 . 40 1 5 18 NU 1*

1 7 7 0 1394.86 6 . 40 1 5 16 NU 1*

7 6 0 6 446 .71 5.990506 2NU2*

0 1 1 1 37.13 1 . 244747 2NU2

2 8 6 3 1411.65 5. 144364 NU 1*

6 7 0 7 586.26 1,838288 2NU2*

4 5 3 3 504.00 0 , 863 547 2NU2

6 9 2 7 1201 .95 6,247031 2NU2*

0 3 2 1 212.15 1,092505 2NU2**

5 6 1 6 447 . 24 1.783035 2NU2**

1 4 2 2 315.79 2.167225 2NU2

0 7 7 1 1394.86 6.401518 NUl

1 7 7 0 1 394 . 86 6.401516 NU 1 2 4 2 3 300 .35 1 .848533 2NU2*

6 9 4 5 1 360 .28 1 . 797448 NU 1 3 8 6 2 1411 .68 5 . 142711 NU 1 2 8 6 3 1411 .65 5. 144364 NUl

5 5 2 4 416.22 2.671788 2NU2*

7 10 1 10 1114.56 0.015027 2NU2

17
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm-i cm-1

gm cm-2

cm-1

otm.

3284.8 3 0.0085 0.0631 7 0 7

3285.01 0 . 1492 0.0623 8 2 7

3285 . 69 0.0046 0 ,0984 3 2 2

3285.70 0 .0092 0,0717 4 1 3

3286.20 0 .0028 0 , 0642 7 1 7

3286.22 0.3507 0,0602 8 0 8

3286.75 0,0013 0,0671 7 1 3286.79 0.0044 0,0679 9 3 6

3287.15 0,0016 0,0830 3 3 1 3287.55 0.0013 0,0681 7 3 5 3288 . 47 13,5567 0,08 54 3

o. 0

3288 . 9 1 6,8306 0.0710 6 2 5 3289.43 0,0075 0.0803 5 3 3

3289.47 0,0032 0.0781 7 2 6

3289.49 0.0051 0.0818 7 3 5

3289.94 0.0013 0 . 0799 1 4

3290 .35 0.5458 0.0 759 8 2 6

3290,50 0.00 55 0. 0829 3 2 3290.76 0,0015 0 . 0843 6 1 5 3291 . 35 22 ,9399 0 . 0631 7 0 7

3292 .51 12 ,3883 0. 0984 3 2 2

3292.65 0,5516 0.0834 9 3 6

3292 .70 0.0268 0 .0646 5 5 1 3292 .76 7.6787 0. 0642 7 1 7

3292 .80 0.6267 0 .0799 5 1 4

3293.04 3.5190 0.0671 7 1 6

3293.22 0 .0063 0 .0636 7 2 6

3293 . 40 0, 1771 0.0750 8 3 6

3293.43 0,0010 0.0659 10 3 7

3293 . 66 0,0017 0.0679 5 3 3

3293 .73 0,0806 0.0590 5 5 0

3294. 11 0,2648 0.0708 8 4 4

3294. 18 4,4189 0.0830 3 3 1 3294.63 0,0023 0.0601 7 2 6

3294. 89 0,0015 0.0629 11 3 8

3294 . 96 0.0597 0.0955 2 3

3295 . 22 0.0090 0.0520 8 0 8

3295.82 0 ,001

5

0.0603 8 3 6

3295.84 0,0269 0.0523 8 1 8

3296.09 0,0020 0,0561 10 2 8

3296. 13 0 ,4497 0,0848 7 3 4

3296.34 0,0014 0.0803 5 3 3

3296.84 3,9939 0.0843 6 1 5

3297.07 0 ,0506 0,0587 8 6 3

3297 . 49 14,7987 0.0829 3 2

3297 .58 0,0649 0.0766 9 3 6

3297.83 0 ,0354 0 .0648 7 4 4

3298. 11 0,6557 0.0681 7 3 5

3298.27 0,0027 0.0643 6 4 3

3298.35 0 ,00 12 0 .0697 5 3 2

3298 .37 0,0135 0.0751 6 3 4

3299 . 74 0,1073 0. 0688 7 4 3

3299.91 0,0449 0.0961 3 2 1 3300.31 0,3378 0.0535 5 4 2

J" Kc E" L BAND

cm *

6 1 6 447.24 5.933681 2NU2^^*

9 4 6 1340.89 0.038564 NU3

2 1 1 95. 17 1.666667 2NU2**

5 5 0 742 . 10 0,000091 NU3

6 0 6 446.71 5,990506 2NU2**

9 2 7 1201.95 0,034667 NU3

7 0 7 586.26 1,838288 2NU2**

9 6 3 1631.41 0,039684 NUl

3 2 2 206. 30 1,035682 2NU2**

8 5 4 1255.16 0,084527 NU3*

3 2 1 212.15 1,092505 2NU2

6 1 6 447. 24 1,783035 2NU2

5 2 4 416.22 2,492169 2NU2*

6 1 5 2146.28 4,008107 2NU2***

8 0 8 744.09 0,017472 2NU2

6 4 3 756.75 0,071290 NUl*

8 1 7 882.93 3,773034 2NU2

4 2 3 300.35 1,8,48 5 33 2NU2**

5 2 4 416.22 2.671788 2NU2**

6 1 6 447.24 5.983681 2NU2

2 1 1 95. 17 1.666667 2NU2

9 2 7 1201 .95 6.247031 2NU2

6 4 2 757.78 0.098971 2NU2

6 0 6 446 .71 5.990506 2NU2

6 4 3 756.75 0.071290 NUl

7 0 7 586.26 1.838288 2NU2

7 5 3 1059.65 0.009705 NUl

7 4 3 931.22 0. 519243 2NU2

10 6 4 1875.53 0.095771 NUl

6 5 2 2552.85 0. 105000 NU3***

6 4 3 756.75 0.098702 2NU2

9 5 5 1474.99 3.26 NUl3 2 206.30 1.035682 2NU2

7 1 7 586.48 1.816721 2NU2-M11 6 5 2144. 12 0. 189337 NUl

3 1 2 173.36 1.970843 2NU2*

7 1 7 586.48 6.998008 2NU2*

8 2 7 2495.18 3.456295 2NU2***

7 0 7 586.26 7.000291 2NU2*

10 6 5 1875.00 0.005881 NU3

6 4 3 756.75 0.550367 2NU2

5 2 4 416.22 2.492169 2NU2**

5 2 4 416.22 2.671788 2NU2

9 5 4 1477.31 2.26 2NU2 +

4 2 3 300.35 1.848533 2NU2

10 5 5 1724,72 0.261892 NU3

6 5 1 888,63 0.250934 2NU2

8 5 4 1255.16 0.084527 NU3

7 5 2 2724. 19 4. 131192 NUl***

6 5 1 2552 .87 0.221000 NU3***

6 2 5 552.92 2.963539 2NU2*

6 5 2 888 .60 0.253734 2NU2

2 1 2 79.48 0.925282 2NU2*

6 6 1 1045.07 0.015207 NU3

18
LINE HALF

FREQUENCY STRENGTH WIDTH J' K a ^ m —

1

1 1 * cnn~i cm"^

UI ( 1 Li ' 1 2 atm.

3300.39 0.0492 0.0549 8 6 2

3300.46 0.1127 0.0540 5 4 1 3300.78 0.0073 0.0530 12 3 9

3301.79 0.0017 0.0520 8 0 8

3301.83 0.0111 0.0955 4 2 3

3302.43 0.0050 0.0523 8 1 8

3302.70 0.0074 0.C758 8 4 5

3302.72 0.4661 0.0784 7 2 6

3303.25 3.7326 0. 0803 5 3 3

3303. 53 0.0054 0.0757 7 4 4

3304.44 0.0058 0.0770 8 3 6

3304. 54 0.0212 0.0760 9 3 7

3304.63 0.0089 0.0644 7 1 7

3305.20 0.0025 0.0751 6 3 4

3305.36 0.0054 0.0646 8 2 7

3306.01 0.0011 0.0542 8 1 7

3306. 11 0.0028 0.0790 6 1 6

3306.45 0.0094 0.0498 6 5 2

3306.46 0.0031 0.0499 6 5 1 3306. 59 0.0083 0.0961 3 2 1 3307.65 0.0043 0.0859 7 2 5

3307.67 1 . 1631 0.0601 7 2 6

3307.72 0.0164 0.0770 10 3 8

3308.03 0.9571 0.0665 7 4 4

3308.36 4.4811 0.0520 8 0 8

3308.40 0.0189 0.0791 3 1 3

3308.70 29.8740 0.0955 4 2 3

3309.02 13.4655 0.0523 8 1 8

3309. 16 0.0149 0.0927 5 2 4

3309.82 0.0026 0.0507 9 1 8

3310.50 4.6862 0.0498 6 5 2

3310.51 1.5622 0.0499 6 5 1 3310.78 0.0202 0.0664 6 2 5

3311.00 0.0533 0.0747 10 3 7

3311.24 0.0252 0.0756 6 4 3

3311.35 0.0140 0.0436 9 0 9

3311 .66 0.0047 0.0437 9 1 9

3312.03 6.7403 0.0751 6 3 4

3312.99 0.0059 0.0686 7 4 3

3313.27 22.4584 0.0961 3 2 1 3313.43 1 .4190 0.0790 6 1 6

3313,82 0.0174 0.0734 7 1 6

3314.03 0.0376 0.0616 11 3 8

3314.51 0.0032 0.0503 8 2 7

3314.51 0.0013 0.0578 10 1 10

3315.07 0.4359 0.0768 8 3 5

3315. 12 0.0011 0.0686 7 4 3

3317.26 2.9302 0.0686 7 4 3

3317.69 0.1444 0.0806 4 1 3

3317.72 0.0046 0.0614 11 2 9

3317.96 0.0026 0.0436 9 0 9

3318.38 0.0605 0.0783 5 0 5 3318.53 2.1333 0.0859 7 2 5

3318.77 0.5373 0.0542 8 1 7

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cm"'

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6 6 0 1 045 . 0 ^ 0.015215 Ml 11 NU3

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19
LINE HALF

FREQUENCY STRENGTH WIDTH J' K Q

1 cm ' cm"' cm~i

gm cm ~ 2 atm.

3320. 10 0.0032 0.0734 7 1 6

3320. 13 0.0021 0.0782 7 3 5

3320. 13 0.0023 0.0876 7 4 3

3320. 14 0.0012 0.0640 4 3 2

3320.24 0.6037 0.0646 9 2 7

3320.48 0.0031 0.0539 9 0 9

3321 . 43 0.0038 0.0645 4 3 1 3321.77 0.0454 0.0863 10 4 6

3321.83 0.0148 0.0842 3 3 1 3321.92 0.0774 0.0640 8 4 5

3322.24 0.0037 0.0811 5 0 5

3322.58 0.0050 0.0553 7 6 2

3322.87 0.0309 0.0873 6 2 5

3322.99 7.4432 0.0927 5 2 4

3323. 12 0.0442 0.0840 3 3 0

3323.25 0.1319 0.0772 9 2 7

3323.34 0.0151 0.0527 7 6 1 3323.45 0.0055 0.0500 7 5 3

3323.55 0.0165 0.0502 7 5 2

3323.98 1 .1378 0.0682 7 3 5

3324.44 0,0013 0.0604 5 4 2

3324.57 7.0249 0.0436 9 0 9

3324.89 2,3430 0.0437 9 1 9

3325.60 0 .0034 0.0776 6 3 4

3325,79 0.0030 0.0603 8 3 6

3325.82 0.0020 0.0729 8 1 7

3325.94 0.0525 0.0684 10 3 7

3325 . 97 0.0079 0.0800 5 4 2

3326. 12 1 .0554 0.0782 7 3 5

3326.38 8.6781 0.0734 7 1 6

3326.68 0.0268 0.0741 8 4 4

3326.76 0.0022 0.0381 10 0 10

3326.80 0.9873 0.0648 7 1 7

3326.91 0.0066 0.0381 10 1 10

3326.97 0,0014 0.0840 6 4 2

3327.34 1.8748 0.0811 5 0 5

3327.54 0.0019 0.0839 6 2 5

3327. 55 1 .6097 0.0503 8 2 7

3327.57 0.4073 0.0684 6 3 4

3328.67 0.0207 0.0653 12 4 9

3328.94 0.4264 0.0887 9 4 5 3329.66 1 .2834 0.0691 7 2 6

3329.78 0.0057 0.0873 6 2 5

3329.79 0.0021 0.0434 9 6 4

3330.00 0.0013 0,0443 9 1 8

3330.11 0.0162 0,0643 6 4 3

3330.78 0.0046 0.0876 7 4 3

3330.95 0.2729 0.0760 7 3 4

3332.37 0.0030 0.0643 6 4 3

3332.66 0.0076 0.0447 5 5 1 3332.66 0.0228 0.0447 5 5 0

3332.70 0.1052 0.0851 8 3 5 3332.98 0.0120 0.0404 12 2 10

3333.07 0.0010 0.0737 9 3 6

I" J K a "^c t

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6 2 5 552 .92 3.799063 2NU2**

8 4 4 1131 .76 2. 323327 NUl*

7 3 4 2462 .87 4. 268667 2NU2***

5 5 1 2406. 15 0. 101300 NU3***

9 1 8 1079 . 07 3 . 674255 2NU2

9 4 6 1340 . 89 0.001797 NU3

5 5 0 2406. 15 0. 11 1100 NU3***

10 3 7 1538 .23 8. 179783 2NU2

2 2 0 1743 .47 2.394805 2NU2***

7 5 2 1059. 85 0.427306 2NU2

6 3 4 648 .97 0.123125 NUl*

8 5 3 1255 .92 0.222252 2NU2

5 1 4 399.46 3. 129447 2NU2*

4 1 3 275.52 2.444582 2NU2

2 2 1 1742 . 28 2 . 366160 2NU2***

10 4 6 1616.51 0. 306915 NU3

8 5 4 1255.16 0.221954 2NU2

6 6 0 1045.07 0. 084869 2NU2

6 6 1 1045 . 07 0. 084894 2NU2

7 2 6 709.60 3.273499 2NU2

6 5 1 2552 .87 2. 56 NU 1***

8 1 8 744 . 16 8 . 007087 2NU2

8 0 8 744.09 8.007851 2NU2

7 4 3 2572.13 2.767638 NU1**»

8 2 7 885.62 3.456295 2NU2*

9 3 6 1282 .92 0. 139840 NU3*

11 4 8 1843.02 4.032477 NUl

6 1 5 542.91 0.009847 2NU2

8 4 4 1131 .76 2.323327 NU 1 6 2 5 552.92 3. 799063 2NU2

7 5 3 1059.65 0.444062 2NU2

9 1 9 920.21 9,013420 2NU2*

8 3 6 1006.12 0. 036269 NU3

9 0 9 920 .18 9,013676 2NU2*

6 3 3 2282 .59 3.075987 2NU2***

6 3 4 648.97 0.123125 NUl

7 3 4 2462 .87 0 . 996364 NU 1***

8 1 8 744. 16 1.833129 2NU2

7 5 3 1059 .65 0.058714 NU3

13 3 10 2414.73 5. 30517 NUl

9 3 6 1282 .92 7. 165263 2NU2

8 4 5 1122 .72 0.08441

1

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5 1 4 399 .46 3. 129447 2NU2**

9 8 1 2009 .87 0.012330 NU3

9 0 9 920 . 18 1.844131 2NU2*

7 5 2 1059.85 4. 131192 NUl*

7 3 4 842.38 4.268667 2NU2*

8 5 3 1255.92 0. 105067 NU3

7 5 2 1059.85 4.131192 NUl**

6 6 0 1045 .07 5. 399693 NUl*

6 6 1 1045 . 07 5. 399718 NUl*

7 4 4 927.77 0.898681 2NU2

13 3 11 2248 . 16 7.87109 NUl

10 4 7 1581 »34 3. 465920 NUl*

20
LINE HALF

FREQUENCY STRENGTH WIDTH J'

gm cm~2

prn — 1 V^l 1

1

fl tm

3333.26 0.0182 0.032 14 0 14

3333.26 0.0546 0.032 14 1 14

3333.31 0.0429 0.033 13 1 12

3333.37 0.0143 0.033 13 2 12

3333.44 0,0022 0.0417 8 6 2

3333. 56 0.0012 0.0381 10 1 10

3333.75 0.0059 0.0787 5 4 1 3334.64 8.0867 0.0643 6 4 3

3334.69 0.0014 0.0447 5 5 1 3334.69 0.0042 0.0447 5 5 0

3334.80 0.0014 0.0655 5 1 5

3336.02 0.0305 0.0470 12 3 10

3336. 18 0.3080 0.0894 8 4 4

3336.24 0.0020 0.0720 4 4 0

3336.69 15.4453 0.0873 6 2 5

3336.73 3 .7934 0.0447 5 5 1 3336.73 11.3802 0.0447 5 5 0

3336.86 0. 5024 0.0737 9 3 6

3337. 10 0.0690 0.0683 8 0 8

3337.34 0.0059 0.0689 4 4 1 3337.46 0.0065 0.0781 7 2 6

3337.75 0.0020 0.0719 5 4 2

3337.85 0.0054 0.0656 6 4 2

3337.86 0 .0041 0.0720 6 4 3

3338.43 0.0026 0.0733 6 3 3

3339.00 1.5020 0.0603 8 3 6

3339.08 0.0523 0.0699 6 1 6

3339.30 0.1549 0.0784 3 1 2

3339.36 0.0027 0.0840 6 4 2

3340.07 1 .0982 0.0381 10 0 10

3340.22 3.2949 0.0381 10 1 10

3340.30 0,0431 0.0655 11 3 8

3340.40 0.0034 0.0613 8 1 7

3340.51 0.0073 0.0970 4 2 2

3341.36 0.9587 0.0729 8 1 7

3342.03 0.0046 0.0558 9 1 8

3342.28 2.7098 0.0656 6 4 2

3342. 38 0.0047 0.0962 5 2 3

3342.93 0.6747 0.0443 9 1 8

3343.27 0.0296 0.0868 4 3 2

3344.28 0.0056 0.0649 10 2 8

3344. 35 0,0012 0.0781 7 2 6

3344.42 0,0010 0.0775 8 3 5

3345.08 0,0136 0.0620 9 4 6

3345.24 0.0119 0.0787 5 4 1 3345.45 0.0104 0.0679 5 3 3

3345.96 2 .3073 0.0876 7 4 3

3347.25 0.0155 0.0515 6 6 1 3347.29 0.0099 0.0834 4 4 1 3347.70 0.0052 0.0497 6 6 0

3347.96 0.2250 0.0430 9 2 8

3348. 15 0,0039 0.0720 4 4 0

3348.20 1 .3374 0.0733 6 3 3

3348.39 0,5063 0.0775 8 3 5

J" Kc E" L BAND

cm-1

15 1 15 2358.44 14.00193 NUl

15 0 15 2358.44 14.00192 NUl

14 2 13 2327.90 11.01049 NUl

14 1 13 2327.88 11 .00954 NUl

8 8 1 1789.10 0.004043 NU3

9 0 9 920 . 18 9.013676 2NU2**

5 3 2 2130.50 2,066632 2NU2*^t7 5 2 1059.85 4,131192 NUl

6 6 0 1045 .07 5,399693 NUl**

6 6 1 1045.07 5,399718 NUl**

5 5 0 742. 10 0.000013 NU3

13 2 11 2246.98 7.82232 NUl

8 3 5 1050. 15 4.85 2NU2-

4 3 1 2005.92 1,088294 2NU2**

5 1 4 399 .46 3, 129447 2NU2

6 6 0 1045 . 07 5, 399693 NUl

6 6 1 1045.07 5, 399718 NUl

10 4 7 1581 .34 3,465920 NUl

8 3 5 1050.15 0, 101 NU1 +

4 3 2 2004.81 1 ,082946 2NU2**

6 1 5 542 .91 4,008107 2NU2*

5 3 3 2126.41 2,024051 2NU2**

7 5 3 1059.65 4, 143594 NUl*

6 3 4 2271 . 70 2,878858 2NU2**

7 5 2 1059.85 0,063852 NU3*

8 2 7 885.62 3.456295 2NU2

6 4 3 756.75 0.005871 NUl

4 4 1 488 . 10 0.004537 NUl

6 3 3 661.56 3.075987 2NU2*

9 1 9 920,21 9.013420 2NU2

9 0 9 920, 18 9.013676 2NU2

1

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7 2 6 709.60 4,913532 2NU2*

3 1 3 142 .28 0,610552 2NU2*

9 3 6 1282.92 0, 139840 NU3

9 5 5 1474.99 0,005298 NU3

7 5 3 1059.65 4, 143594 NUl

4 1 4 1821.61, 0,386397 2NU2**

9 0 9 920.18 1,844131 2NU2

3 2 1 1819. 34 2,320352 2NU2**

10 5 5 1724.72 0,238204 NUl

6 1 5 542 .91 4.008107 2NU2**

9 4 6 1340.89 3.141455 NUl*

8 5 3 1255.92 0. 597432 2NU2

5 3 2 508.81 2.066632 2NU2*

6 5 2

• 888.60 0. 105000 NU3*

7 3 4 842 .38 4.268667 2NU2

7 5 2 1059.85 0.084894 2NU2

5 1 4 399.46 0.001994 2NU2

7 5 3 1059,65 0. 084869 2NU2

9 1 9 920.21 1 .842036 2NU2

4 3 1 383.85 1.088294 2NU2*

7 5 2 1059.85 0.063852 NU3

9 4 6 1340.89 3. 141455 NUl

21
LINE HALF

FREQUENCY STRENGTH WIDTH J' K Q K cm 1 cm ' cm 1 gm cm^ U I 1 1 1.

3 348 .56 0.0692 \j m \J ^ ^ '-r 1 0 C 8

3348 .90 0.0186 n . 0 5 1 6 8 5 4

3349 • 47 0.0095 0.0861 4 3 1 3349 .53 0.0073 0,0687 5 3 2

3349.54 0.0117 0.0689 4 4 1 3349 .79 0.0010 0.0656 8 4 5 3349 .80 0.0062 n . 0 54P 8 3

3349 .88 0.4189 n .069? 7 0 7

3350.01 0.0116 0.0839 6 2 5

3350.09 0.0296 0.0842 3 3 1 3350.22 0 . 0040 0.0719 5 ''h 2

3350.37 0.0113 0.0 545 4 4 1 3350.40 0.0039 0 . 0 546 4 4 0

^ -J ^ \J • (J 0 . 00 PO c; 3 3

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3 3 51.54 0.0884 0*0 840 3 0

3351.80 0 .0029 0.0812 8 2 6

3351 ^ 93 0.0082 0.0720 6 4 3

3352.69 0 .0022 0.0787 5 4 1 3 353.26 1.7229 0.0613 8 1 7

3353.65 3.6532 0,0970 4 2 2

3353.70 0.0178 0*0703 5 2 3

3353.84 0.0108 0 .0646 8 2 7

3354. 19 0.1379 0.0465 1

1

2 9

3354 . 44 1.3721 0.0 840 6 4 2

3355,25 1.3923 0. 0349 1

1

0 1

1

3355.31 0 . 464

1

0 . 0 349 1

1

1 1

1

3355.36 0.0015 0 . 0696 7 4 4

3355 . 44 0.1535 0.032 1

3

0 13

3355 .72 5.1842 0.0 679 5 3 3

3355 .75 0.0511 0-0665 9 1 8

3355.92 0.1955 0.0529 9 3 7

3356.21 0.0208 0 . 0776 6 3 4

3356.27 0. 1577 0.0349 1

2

2 1

1

3356.33 0 .0045 0 .0585 1

1

2 10

3356.56 0 .4977 0.0 793 8 2 6

3356.70 0.0461 0. 0774 9 4 5 3357.00 5 .8196 0.0839 6 2 5

3358.10 0 .0087 0.0796 7 3 4

3358.62 0,0164 n . 0 840 3 3 0

3358.94 0.0038 0 . 0 776 6 3 4

3359.55 3.6412 0.0697 5 3 2

3359.70 0,0172 0.0735 1

1

4 8

33f)0 . 14 5.9457 0.0787 5 4 1 3360.39 0 ,0441 0,0688 9 2 7

3360.66 0,0020 0 . 0646 8 2 7

3360.68 0,0550 0.0557 1

1

3 9

3360.92 0,0165 0.0 729 6 2 4

3361.68 10.3768 0.0776 6 3 4

-J ~/ \J 9 (J n . 0 796 7 3 4

3362.74 0.0106 0.0771 5 3 2

3362.91 1.9510 0.0720 4 4 0

3363.09 0,0164 0.0600 10 4 7

3363. 10 0,0347 0.0608 5 4 1

J" K a '^c E" L BAND

cm-i

10 1 9 1293.04 3.646815 2NU2

7 6 1 1216.20 0.221954 2NU2

3 2 2 1813.81 2, 164905 2NU2***

6 5 1 888.63 0.221000 NU3*

4 3 2 382.52 1 .082946 2NU2*

8 3 6 2630.21 4. 264036 2NU2*^^*

7 6 2 1216.20 0.222252 2NU2

8 2 6 982.91 0.040852 NU3

7 3 4 842.38 0.996364 NUl*

2 2 0 136.17 2. 394805 2NU2*

5 3 3 504.00 2.024051 2NU2*

5 5 0 2406. 15 3.52 NUl*-)^*

5 5 1 2406. 15 3.61 NU1**^<-

6 5 2 888 .60 0. 105000 NU3*^-<-

6 1 5 542.91 4.008107 2NU2

2 2 1 134.91 2.366160 2NU2*

9 4 5 1360.28 0. 309042 NU3*

6 3 4 648 .97 2.878858 2NU2*

5 3 2 508 .81 2.066632 2NU2-^*

7 2 6 709.60 4.913532 2NU2

3 1 3 142. 28 0.610552 2N'J2

5 5 0 742.10 0.001850 NUl

7 1 6 704.22 4.996649 2NU2-^

12 3 10 1962 .55 7.003088 NUl

6 3 3 661.56 3.075987 2N'J2

10 1 10 1114.56 10,018153 2NU2

10 0 10 1114.55 10.018239 2NU2

7 3 5 816.72 3.637027 2NU2*

14 1 14 2073 .66 12.99957 NUl

6 5 2 888.60 0. 105000 NU3 +

9 4 5 1360.28 0. 116860 NUl

9 2 8 1080.38 3. 554957 2NU2

7 4 3 931 .22 2.767638 NUl^^

13 1 12 2042.33 9.99731 NUl

1

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4 7 1899.06 0.013267 NU3

7 3 5 816.72 2.422109 2NU2

8 5 4 1255.16 0.669979 2NU2

7 3 4 842 .38 0.996364 NUl

8 4 5 1122 .72 3.022183 NUl*

2 2 1 134.91 2.366160 2NU2**

7 4 3 931.22 2.767638 NUl->^*

6 5 1 888 .63 0.221000 NU3 + 12 3 9 2105.90 4. 355455 NUl

5 3 2 508.81 2.066632 2NU2

9 5 4 1477.31 0. 180415 NUl

7 1 6 704.22 4.996649 2NU2^f*

12 2 10 1960.22 6,964699 NUl

6 5 1 888 .63 • 0.010677 NUl

7 4 3 931 .22 2.767638 NUl

8 4 5 1122.72 3.022183 NUl

6 4 3 2398.39 3.53 NUl***-

4 3 1 383.85 1 .088294 2NU2

9 5 4 1477.31 0.720783 2NU2

6 5 2 888.60 3.63 NUl*

22
LINE HALF

FREQUENCY STRENGTH WIDTH J' K

crn~' gm crn~2 atm.

3363. 15 0.0028 0.0695 8 5 4

3363.80 0.0075 0.032 14 1 13

3363.82 0.0025 0,032 14 0 14

3363.85 0.3093 0.0907 3 3 0

3364.23 5 ,8655 0,0689 4 4 1 3364.27 0.2108 0.0803 4 0 4

3364.31 14,8187 0,0842 3 3 1 3364.77 1 .4440 0.0812 8 2 6

3364.88 1 .9911 0.0719 5 4 2

3365.36 0,0064 0.0608 5 4 1 3365.45 0,0306 0.0590 8 0 8

3365.71 44,2161 0.0840 3 3 0

3366. 12 0,0020 0.0874 4 0 4

3366. 15 0.0859 0.0382 10 1 9

3366.23 0.0754 0.0734 7 2 5

3366.49 4. 1179 0.0720 6 4 3

3366.99 0.0242 0.0712 8 2 6

3367.22 0.0021 0.0840 6 2 4

3367.34 0.0223 0.0743 5 1 5

3367.49 5,4234 0.0646 8 2 7

3367.62 17,3426 0.0608 5 4 1 3368.72 0,2578 0.0378 10 2 9

3368.80 2,3502 0.0744 6 2 5

3369. 10 3,9693 0.0604 5 4 2

3369. 12 0.0311 0.0608 8 1 7

3369.74 0.7503 0.0696 7 4 4

3369.91 0.1768 0.0332 12 0 12

3369,93 0.5304 0.0332 12 1 12

3370.98 1 ,0166 0.0874 4 0 4

3371.36 0,0593 0.0868 4 3 2

3371.69 0,0018 0.0539 9 2 8

3371.88 0,1900 0.0820 9 3 6

3372.81 0,0070 0.0640 4 3 2

3373.15 0,0023 0. 0864 5 2 4

3373.97 0,1651 0.0544 10 2 8

3374. 18 0,0230 0.0645 4 3 1 3374.32 0 .0041 0.0529 9 5 5

3374.34 0.2056 0.0458 10 3 8

3374.69 1 .6486 0.0868 5 1 5

3375.35 0,0124 0.0586 9 5 4

3375.65 1 ,0261 0. 0656 8 4 5 3375.68 0.0098 0.0896 6 3 4

3376. 57 0,0032 0.0515 11 5 7

3376.64 0.1926 0,0892 4 3 1 3377.09 0,0021 0.0459 8 7 2

3377.49 2,6321 0.0507 9 1 8

3377.94 0,0013 0. 0640 4 3 2

3378. 03 0,5830 0.0324 12 1 12

3378.31 0,0190 0.0861 4 3 1 3378.41 0,1905 0.0325 12 0 12

3378.47 0.0217 0.0628 9 1 9

3378.51 0.0153 0. 0884 5 3 2

3378. 52 0.0110 0.0868 4 3 2

3378.54 0,0015 0.0794 6 0 6

J" U E" L BAND

cm"!

9 2 7 1201 .95 0,030877 2NU2

14 2 13 2327.90 1 , 90878 NUl

14 1 13 2327 .88 1 , 90883 NUl

3 0 3 136.77 0.016715 2NU2

4 3 2 382 .52 1 . 082946 2NU2

5 4 1 610.35 0.001060 NU3

2 2 0 136.17 2.394805 2NU2

9 4 5 1360 .28 0. 309042 NU3

5 3 3 504 . 00 2 . 024051 2NU2

6 5 2 888.60 3. 63 NUl->^*

8 4 5 1122.72 0.001991 NU3

2 2 1 134,91 2.366160 2NU2

5 3 3 504.00 0. 095779 NUl*

10 0 10 1114.55 1 .848326 2NU2

7 5 2 1059.85 0.038149 NUl

6 3 4 648 .97 2.878858 2NU2

8 5 3 1255 ,92 0.098024 NUl

7 3 2572,13 0.157817 NU3-^**

5 4 2 610.12 0.003573 NUl

7 1 6 704.22 4, 996649 2NU2

6 5 2 888.60 3.63 NUl10 1 1 0 1114,56 1.847651 2NU2

7 4 4 927,77 0. 173000 NU3 +

6 5 1 888 ,63 2 . 56 NUl8 5 4 1255,16 0.003922 NU3

7 3 5 816,72 3.637027 2NU2

1

1

1 1

1

1327, 14 11.021861 2NU2

1

1

0 11 1327,14 11 .021891 2NU2

5 3 3 504 , 00 0 . 095779 NUl

3 2 1 212.15 2 .320352 2NU2*

8 1 7 882 .93 6.019178 2NU2*

8 4 5 1122,72 1 .416234 2NU2

5 5 1 742 ,10 0. 10 1300 NU3*

6 3 3 2282 , 59 1.411171 NUl***

1

1

3 9 1695 .03 5.954956 NUl

5 5 0 742. 10 0. 111100 NU3*

8 6 2 1411 .68 0. 391 127 2NU2

10 2 9 1293 .66 3. 605841 2NU2

6 2 4 602 .77 0. 254241 NUl

8 6 3 1411.65 0.393126 2NU2

8 3 6 1006 . 12 4.264036 2NU2

5 2 3 2053.98 2.452523 2NU2***

1

1

7 4 2321 .94 0 .077402 NU3

4 0 4 222 . 06 0. 047652 2NU2

9 6 3 1631.41 0. 197898 2NU2

8 2 7 885 .62 5 ,987889 2NU2

5 5 1 742 . 10 0, 101300 NU3**

13 0 13 1806.78 11, 99672 NUl

3 2 2 206 .30 2 , 164905 2NU2*

13 1 13 1806,78 11.99676 NUl

9 3 6 1282 ,92 0.003124 NU3

4 2 3 1907 ,99 1.841317 2NU2***

3 2 1 212,15 2.320352 2NU2**

7 2 5 2392,58 0.051494 NU3***

23
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq K cm ' gm cm~^ n tm

3378 ,79 0 . 5041 0,0361 1

1

1 10

3379. 10 0.1680 0 , 0379 1

1

2 10

3379. 12 0,9184 0. 0731 6

"1 6

3379.27 0,0043 0.0645 3 1 3379.52 0,0026 0,0424 8 6 3

3380.41 2 .7376 0.0790 6 3 3

3381. 13 0.0659 0. 0442 1

1

2 9

3381 . 36 0.0017 0.0698 9 2 7

3381 .67 0 .0068 0.0734 4 3 1 3381 . 87 0.0022 0. 0804 5 1 5

3382.87 0.0151 0.0516 9 5 5 3383.07 3 .4956 0. 0640 4 3 2

3383.14 0 .0204 0.0733 4 3 2

3383 .74 0 .0605 0.0324 13 1 13

3383 .74 0.1814 0.0324 13 0 13

3383.87 0 .0026 0.0804 7 1 6

3384. 37 1 1 . 5062 0.0645 4 3 1 3384. 73 0.1328 0 .0600 9 4 6

3385.01 0.0074 0.0785 10 4 6

3385.24 0.8958 0.0539 9 2 8

3385.27 0 .0071 0.0498 8 5 4

3385.35 0 .0035 0.0861 4 3 1 3385 . 44 0.4891 0.0655 10 3 8

3385.69 29.6440 0. 0868 4 3 2

3385.98 0.0051 0.0538 9 5 4

3386 .30 0.0215 0.0509 8 5 3

3386.62 0.0101 0.0325 13 1 13

3386.67 0.0303 0.0327 13 0 13

3387.26 0.0896 0.0348 11 1 10

3387.36 0.0184 0. 0769 5 3 3

3387.72 0.0066 0.0563 10 5 5

3387.81 0.0189 0. 0476 7 5 3

3388 .05 0 .0063 0.0479 7 5 2

3388.46 0,0299 0. 0348 1

1

2 10

3389. 17 0,0028 0.0795 7 2 5 3389. 18 0,0119 0.0892 5 3 3

3389.23 0.0093 0.0962 5 2 3

3389 .31 0,0153 0.0656 7 1 6

3389.46 0 ,0424 0. 0762 4 1 4

3389.87 0 ,1961 0 . 0741 7 0 7

3389. 96 0 ,0034 0.0769 5 3 3

3390.68 0,0024 0 , 0444 10 2 9

3391 . 54 1 .4140 0.0637 9 2 7

3392. 09 0.0677 0, 0709 8 1 7

3392.40 9.5122 0,0861 4 3 1 3392. 57 9.2083 0.0769 5 3 3

3392 .70 11.7236 0.0546 4 4 0

3392.95 34.2967 0.0 545 4 4 1 3393 ,19 0,8539 0.0698 9 2 7

3394. 24 0 , 1346 0.0 536 10 4 7

3394 , 54 0,1520 0.0811 10 4 7

3394. 87 0,0220 0.0406 1

1

3 9

3395.66 0.0017 0.0962 5 2 3

3395.88 0.0052 0.0793 11 5 7

J" E L BAND

cm-i

12 2 11 1774.74 9,078065 NUl

12 1 11 1774. 60 9.076485 NUl

7 3 5 816.72 0.038676 NU3

5 5 0 742. 10 0. 111100 NU3**

7 7 0 1394.86 0.074321 2NU2

7 4 4 927.77 2.14 NUl11 1 10 1524,87 3.646421 2NU2

8 3 6 1006, 12 3. 529968 2NU2*

5 4 2 2251.71 3.270203 NUl*^^*

6 3 4 2271,70 0.038984 NU3*i<-»

9 7 2 1810,63 0.029706 NU3

5 5 1 742, 10 0.101300 NU3 +

5 4 1 2251 ,86 3.250024 NUl**-5«-

12 0 12 1557.91 11.99676 2NU2

12 1 12 1557,91 11.99672 2NU2

8 3 5 1050. 15 0. 180748 NU3*

5 5 0 742. 10 0. 111100 NU3 +

9 3 7 1216,27 4,734521 2NU2

9 5 5 1474,99 0,959644 2NU2

8 1 7 882,93 6,019178 2NU2

8 7 1 1590.74 0,014493 NU3

3 2 2 206.30 2, 164905 2NU2**

1

1

2 9 1690.70 5,859437 NUL

3 2 1 212,15 2,320352 2NU2

9 7 3 1810,63 0,029861 NU3

8 7 2 1590,74 0,014513 NU3

13 2 12 2042,38 1,90640 NUl

13 1 12 2042 ,33 1,90653 NUl

11 0 11 1327, 14 1 , 851910 2NU2

6 4 2 757,78 3,066224 NUl*-

10 7 4 2054,40 0,051622 NU3

7 7 0 1394,86 0,004734 NU3

7 7 1 1394,86 0,004736 NU3

11 1 11 1327,14 1,851690 2NU2

8 3 6 2630,21 3,262769 NUl***

4 2 2 315,79 2,324407 2NU2*

4 1 4 224.83 0.386397 2NU2*

7 5 3 1059.65 0.002162 NU3

4 4 1 488 . 10 0.001222 NUl

7 3 4 842 . 38 0.033256 NUl

6 4 2 757.78 3.066224 NUl**

9 1 8 1079.07 7.043661 2NU2*

10 3 8 1446.16 4,932263 NUl

8 4 4 1131.76 0, 146118 NUl

3 2 2 206.30 2, 164905 2NU2

5 4 2 757,78 3,066224 NUl

5 5 1 742.10 3,61 NUl5 5 0 742.10 3.52 NUl8 3 6 1006. 12 3. 529968 2NU2

10 3 8 1446. 16 5,051335 2NU2

1

1

3 8 1813,26 3.178818 NUl

11 2 10 1525,13 3.632655 2NU2

4 1 4 224,83 0.386397 2NU2**

12 4 8 2205,65 1.975180 NUl

24
LINE HALF

FREQUENCY STRENGTH WIDTH J' K J" cm~i cm"i

qm cm~2 atm.

3396 .23 1 .2212 0.0841 7 2 5 8

3396 . 43 0,0022 0.0892 5 3 3 4

3396 . 82 0.0138 0 , 0 864 5 2 6

3397 .21 32,0157 0.0771 5 3 2 6

3397 .28 0,0193 0,032 14 0 14 1 3

3397 .28 0.0578 0.032 14 1 14 13

3397.40 0.4548 0.0880 5 3 2 5 3397 .59 0.0062 0.0532 10 5 6 9

3397 .93 0.0088 0.0794 6 0 6 7

3398 . 42 0.0024 0.0832 8 3 6 7

3398 .81 1 .3424 0 . 0804 7 1 6 8

3399.68 0 .0045 0. 0348 9 8 1 9

3399 . 84 0.0026 0, 0447 9 6 3 8

3400.05 0,0025 0,0864 5 2 4 6

3400 .28 0,0015 0. 0348 9 8 2 9

3400 .32 0,3918 0,0431 10 1 9 9

3400 .65 0,5258 0 , 040

1

10 1 9 1

1

3400 • 73 0 ,0021 0.0619 10 5 5 9

3400.83 0,0021 0.0835 6 2 7

3401 .02 0,6015 0.0331 1

1

1 11 12

3401 . 02 1 ,8044 0.0335 11 0 11 12

3401 . 19 0 .0029 0.0795 2 2 5

3401 . 5

1

1 .5770 0, 0442 10 2 9 1

1

3401 .53 0 ,0024 0.0716 8 2 6 9

3402 .10 4,6556 0 . 0962 5 2 3 4

3402 .18 0.0379 0 . 0694 6 1 5 6

3402 .72 0,0334 0 .0795 3 0 3 4

3403.29 6 ,8788 0. 0864 5 2 i\ 6

3403.68 5,9268 0 .0892 5 3 3 4

3403 .76 0 ,0196 0 • 0896 6 3 4 5

3404.2

1

0 ,0060 0.0890 3 0 3 4

3404.21 1 .1866 0,0444 10 2 9 9

3404. 27 0.0017 0.0539 12 9 12

3405 .02 0 .0270 0, 0646 7 0 7 7

3405 . 51 0.0016 0 • 0 794 6 0 6 7

3406 .64 1 .2173 0,0716 8 2 6 9

3407 .40 0,0063 0,0379 1

2

2 10 1 2

3407 . 84 0,0044 0 . 0694 5 1 4 5

3407,97 0 ,0017 0 .0348 10 1 10 1

1

3408 .11 0,0331 0.0752 10 3 7 9

3408 .17 0,0128 0.0840 6 2 4 7

3408 • 54 0 ,0306 n • 0884 5 3 2 4

3408 . 72 1 .4741 0.0774 5 2 4 6

3408 .83 3.0175 0.0890 3 0 3 4

3409 . 09 0 , 0094 0,0331 12 1 1

1

1 2

3409. 19 0,0395 0,0683 3 3 0 4

3409. 54 0,0131 0, 0680 3 3 1 4

3409.67 0,0283 0,0331 12 2 11 12

3410.07 0.1040 0,0337 12 1 12 12

3410. 19 0 .1288 0. 0552 1

1

6 5 12

3410. 44 0.005 2 0-03? 1 5 1X X1 5 1X 4" 341 0 . 44 0,0156 0 . 03P 1 5 0 1 5 1X 4^ 3410.59 0,0347 0.0337 12 12 12

3411.02 0.0096 0.0622 10 2 9 10

K Q E" L BAND

cm~'

4 4 1131 .76 0.247061 NU3

2 2 315.79 2.324407 2NU2**

3 3 661,56 1.411171 NUl*

4 3 756,75 3. 53 NUH1 13 1806,78 12.99955 2NU2

0 13 1806.78 12.99957 2NU2

0 5 325.35 0.062476 2NU2

6 3 1631.41 0. 576235 2NU2

2 5 782.40 0.051494

2 5 2392.58 3.262769 2NU2>-**-

3 5 1050.15 0. 180748 NU3

9 0 2225,56 1 ,131403 NUl

7 2 1590.74 0, 197898 2NU2

3 3 661 .56 1,411171 NUl**

9 1 2225.56 1 ,131403 NUl

2 8 1080.38 7,032041 2NU2 -

2 10 1525.13 8,063213 NUl

6 4 1631 ,27 0, 586260 2NU2

3 5 2439,97 2,751216 NUl***

0 12 1557,91 11,021861 NUl

1 12 1557,91 11,021891 NUl

4 1 2251 ,86 0,042579 NU3***

1 10 1524,87 8,058917 NUl

3 7 1216,27 4,004942 NUl*

1 4 224,83 0.386397 2NU2

5 2 888 ,60 0.000758 NU3

4 0 488, 13 0.000270 NU3

3 3 661 .56 1.411171 NUl

2 2 315,79 2. 324407 2NU2

2 3 446.50 2.452523 2NU2*

3 2 382.52 0.051049 NUl*

1 8 1079.07 7.043661 2NU2

6 6 2437.56 0. 124675 NU3

4 4 927.77 0.001966 NU3

2 5 782.40 0.051494 NU3**

3 7 1216.27 4.004942 NUl

1 11 1774,60 3.652921 2NU2

5 1 742,10 0.000125 NU3

0 11 2915.94 10.018153 NUl***

4 6 1340 .89 2. 171641 2NU2

4 3 931 .22 0.157817 NU3*

2 3 300.35 1.841317 2NU2*

4 3 756.75 0.015200 NU3-

3 2 382.52 0.051049 NUl

0 12 1557.91 1.854934 2NU2

4 1 2129.63 3.393148 NUl***

4 0 2129.65 3.390390 NUl***

1 12 1557.91 1.854861 2NU2

2 11 1774.74 1.854861 NUl

6 6 2437,56 9.054429 NU3

0 14 2073.66 14.00192 2NU2

1 14 2073.66 14.00191 2NU2

1 11 1774.60 1.854934 NUl

4 6 1616.51 0,021601 NU3

707-944 O - 64 - 3 25
LINE HALF

FREQUENCY STRENGTH WIDTH J' K

Lin * — I LIN gm cm ~ 2 0 tm.

3411 . 10 0.0036 0,0896 6 3 4

3411. 13 0 .0193 0,0871 4 2 3

3411.83 0.0045 0,0869 6 1 5 3411.85 0.3863 0,0516 11 6 6

3411.90 0.4713 0,0747 9 3 7

3412. 1

1

0 .0022 0,0887 6 3 3

3413.09 0.0050 0,0351 13 2 12

3413.09 4.3976 0.0794 6 0 6

3413.77 0.1431 0.0721 11 5 6

3413.84 0.0024 0.0840 6 2 4

3414.23 0.0150 0.0470 13 1 12

3414.48 0.0128 0.0852 5 2 3

3414.65 0 .0020 0.0757 3 2 2

3414.81 0.0130 0.0804 5 1 5 3414.93 0 .0026 0.0806 6 5 2

3414.94 0.0171 0.0795 7 2 5 3415.38 0.1234 0.0733 4 3 2

3415.46 0.4965 0.0566 12 3 9

3415.47 0.0057 0.0884 5 3 2

3415 .49 0 .0249 0.0813 10 5 5 3415 .61 0.1625 0, 0488 12 4 9

3415.97 0.0034 0,0881 7 3 5 3416.00 0.0088 0. 0463 9 1 8

3416.26 0.0190 0.0368 12 3 10

3416.33 0.0042 0.0412 10 7 3

3416.33 0.0126 0.0412 10 7 4

3416.71 0.0415 0.0734 4 3 1 3417.22 0.5182 0.0748 7 1 6

3417.44 0,0029 0.0534 9 2 8

3417.45 0.0032 0.0795 7 2 5 3417.93 0,0228 0.0733 4 3 2

3418.45 9,8020 0,0896 6 3 4

3419.18 0,0016 0,0463 9 1 8

3419.22 0.0077 0,0734 4 3 1 3419.36 0 ,0096 0.0561 11 4 8

3419.52 6.4141 0, 0840 6 2 4

3419.96 8 ,5676 0,0795 7 2 5 3420.03 0,0116 0,0391 9 7 3

3420.03 0,0348 0,0392 9 7 2

3420.49 61,6930 0,0733 4 3 2

3420.74 0,4658 0,0378 11 1 10

3421.37 0,0024 0,0804 5 1 5

3421.74 20,7259 0.0734 4 3 1 3422.25 0,0156 0.0595 1 1 3 9

3422.37 4«3866 0.0463 9 1 8

3422.40 15,2993 0.0884 5 3 2

3422.56 0,1564 0.0385 11 2 10

3423.07 0,4244 0,0564 11 5 7

3423.23 1,7581 0,0354 10 0 10

3423.24 5,2744 0,0348 10 1 10

3423.94 0,0196 0,0369 8 7 1 3423.94 0,0589 0,0369 8 7 2

3424.03 0 ,0334 0,0920 4 1 4

3424. 03 1 ,4699 0,0534 9 2 8

1" F" 1 BAND

5 2 3 446 ,50 2,452523 2NU2**

5 3 2 2 130 , 50 1 , 841317 NU 1

>(><

-7

1 2462,8' 0 , 2 1 4427 NU 3*^^

i 2

/ "7 A A /. 0 A /. A

9 • Oh 0 Oh-O InU 3

1 0 2

Q 1430,00 4, /06625 NU 1

c 2 A- 2024,1

1,411171 2NU2-'-'^-'<-

1 3 3 1

1

2 248 . 16 3 . /^5 3 1 9 NU 1

-77 2 5 782 . 40 0.05 1494 NU3

1 2 5 7 2 300.80 10.04 7055 NU 3

"7

1 4 3 y 3 1 #22 A T CI ~? 0 T ~7 Ml 1 0 J£. ^' NU 3^

i J 2 1 1 2 2ho .90 3 . ' 6 1 3 3 NU 1 6 3 4 2 2 ' 1 . 70 2.452523 NU l-«--»<-* 4 i 2 i 2 9 • 6 3 A A T d C C T 0.015552 Nil 1 0 Jit. ^

[\| (J 3 «- V •><• 6 3 4

^ ^ 0 0 A n / 0,038984 Ml 1 T J' NU 3*

-7

1 0

"7 Q 0 /, r\

f 0 2 • M-0 A A A 0 C T T 0,003511 2 NU 2

Q0 6 1 006 •12 Dm lb c / 69 NU 1 ^

i 0 1 0 • 3 !:> 0 O C A A o y. 3» 2^0024 M 1 I T ii- NU 1

1 3 3 1 0 2 414.73 TT 210/. COA 11 ,684530 NU 3

2 i 3 00.3b 1,84131

7

2 NU 2^*

1 0 1616.51 O M 1 1 A 2 NU 2

i 3

/, 4 1

0

2 426.22 11,4/3010 NU 3

0 2 A T ~7 "7 6 0 2. f / 2, (51216 2 N U 2

1 u 2 9 1293,66 7.043661 ^ 1 1 IT ^i. NU 1^<^

1

2

2 1

1

1774,74 3,6482 29 2NU2

1

0

8 2 2 2 54,34 3,150851 NU 1

1 0 8

03 2 2 54, 34 3, 150801 Ml IT NU 1

I:) /, M- £L 610,12 Q 0 ~7 A O A 0 3«2 / 0203 NU 1

"

( 3 9 3 1 ,22 A T 0 d A A 0. i3!:59oO NU 1

i U 1 1 2 9 3 • Om- 1 A 0 T A /. 1

/ .032041 N U 1 Q 3 D i OOo • 1

2

3»2o2 ^69 Ml IT Al-Al- IN U 1 *

1:3 i D X 0 • 3 5 1 N U 1 ^ *

2 3 2«4t)2!?23 <i NU 2

1

0

2 9 1293 .66 / , 043661 NUl**

5 4 2 610.12 3,270203 NU l*->^ 1

1

6 5 2 144 . 1

2

0,111521 NU3

—J7 4 3 931.22 0,15 '817 Ml 10 NU3

Q0 3 6 1006.12 3,262769 M 1 1 T NU 1 9 8 2 2009.8 7 2, 165389 Mill NU 1 9 8 1 2009.8 1 2, 165395 N 1 1 1 1 NU 1 5 4 1 610.35 0 O CI A A T /. 3 , 250024 M 1 M NU 1

i 0 2 y 12 9 3 .66 Q A Q n 1 "7 8,05891

7

0 M 1 IT 2 INU Z 6 3 4 648.9 7 0,038984 NU 3**

5 4 2 610.12 3 , 270203 M 1 I T NU 1

1 I 5 6 1999.02 A A "7 O / 0 C 0,0 72485 M ! 10 NU 3

1

0

2 9 1293.66 7,043661 NU 1 4 2 3 300.35 1,841317 2NU2

1 0 1 9 1 293 , 04 8,063213 2 NU 2

1 2

r-5

Q T o "7 t y. /. 2 2^5, 44 0 Q r\ Q c; "7 "7 M 1 1 NU 3

i 1 1 1 i L 3 ^ ^ , 1 M- lU,lJ10<i3y in A1QOQQ Mill IN U 1

i 1 0 i i 1 3 ^ r , 1 10.010133 |\U 1 0 8 0 1789, 10 1 . 126216 M 1 1 T In U 1 8 8 1 17 89,10 1. 126215 M 1 1 T NU 1 5 2 3 446 , 50 0.386397 NUl*

10 1 9 1293 ,04 7.032041 NUl

26
LINE HALF

FREQUENCY STRENGTH WIDTH J' K Q K

rrn ~ 1 L-l 1 1 atm.

3424. 32 0.0012 0.0646 6 5 1 3424. 37 0.0016 0.0460 10 6 5

3424.88 0 .0039 0.0580 5 5 0

3425. 12 0 .0013 0.0566 5 5 1 3425.32 0.0036 0.0607 6 5 2

3425.33 0.1336 0.0590 10 2 8

3426. 15 0.3077 0.0772 11 4 7

3426.60 0.0014 0.0866 4 1 4

3426.72 0.2120 0.0794 9 5 4

3426.75 0.2825 0.0446 10 7 3

3426.80 0.0941 0.0425 10 7 4

3426.80 0.0020 0.0580 5 5 0

3427.01 0.0692 0.0865 6 3 3

3427.01 0.0018 0.0607 6 5 2

3427.05 0.0056 0.0824 5 2 3

3427.21 0.0011 0.0620 8 5 4

3427. 34 0.0049 0.0832 8 3 6

3427.54 0.0062 0.0920 4 1 4

3427.77 0.0125 0.0835 6 2 4

3427.93 6.5170 0.0804 5 1 5 3428.43 0.0047 0.0779 4 2 3

3428.61 0.0036 0.0620 8 5 4

3429. 14 0.0099 0.0578 10 4 7

3429.22 0.0061 0.0324 13 1 12

3429.47 0.0046 0.0388 9 0 9

3429. 52 0.0029 0.0333 13 2 12

3429.60 0.0015 0.0382 9 1 9

3430. 30 0.0023 0.0835 6 2 4

3430.40 0 .1349 0 .0943 3 3 1 3430.81 1 .6839 0.0881 7 3 5

3431.06 16 .6946 0.0920 4 1 4

3431.44 0.0084 0.0865 4 2 2

3432.09 0.0012 0.0834 8 3 6

3432.49 0.2575 0.0785 6 1 5 3432.83 6.2277 0.0835 6 2 4

3433. 17 0.1342 0.0863 9 4 6

3433.67 0.0056 0.0349 13 2 11

3433.74 0.2553 0.0793 6 0 6

3433.80 0.1219 0.0358 11 1 11

3434.00 0.0070 0.0834 8 3 6

3434.06 0.3658 0.0359 11 0 11

3434.23 0.0274 0.0869 6 1 5 3434.24 0.1748 0.0756 8 5 3

3434.52 0.0307 0.0674 4 4 1 3434.69 0.0102 0.0665 4 4 0

3435.65 0.0744 0.0590 9 4 6

3435.92 1 .2000 0.0812 10 5 6

3436.05 0.0736 0.0381 12 2 1

1

3436. 12 0.0019 0.0343 13 3 11

3436.22 0.0012 0.0787 5 1 4

3436.29 0.5083 0. 041

1

12 2 10

3436.33 0 . 1892 0 .0330 13 1 12

3436.33 0.5674 0.0330 13 2 12

3436.48 0.1169 0.0871 4 2 3

J K a E L BAND

cm-1

6 4 2 757.78 2.089996 2NU2*

9 7 2 1810.63 0.354752 2NU2

5 4 1 610.35 1. 101100 2NU2*

5 4 2 610.12 1 .100600 2NU2^^

6 4 3 756.75 2.085226 2NU2^'-

9 3 7 1216.27 4. 706625 2NU2

12 4 8 2205.65 10.766337 NU3

5 3 3 2126.41 0.035251 NU3***

9 4 5 1360.28 5. 113359 2NU2

11 7 4 2321 .94 6.588161 NU3

1

1

7 5 2321 .89 6.588139 NU3

5 4 1 2251.86 1. 101100 2NU2**^^

6 0 6 446 .71 0.051901 2NU2

6 4 3 2398.39 2.085226 2NU2***

6 4 2 757.78 0.086601 NU3^^

8 4 5 1122.72 3. 901175 2NU2*

7 2 5 782.40 3.262769 2NU2*

5 2 3 446 . 50 0.386397 NUl**

7 3 5 816.72 2.751216 NUl^-

6 3 4 648 .97 0.038984 NU3

5 4 2 610. 12 0.034972 NU3^«-

8 4 5 2764.71 6.79 NUl-»-**

10 6 4 1875.53 0.086992 NU3

13 0 13 1806.78 1 .90654 2NU2

10 1 10 2705.18 9.013676 NUl***

13 1 13 1806.78 1 . 90640 2NU2

10 0 10 2705.15 9.013420 NUl***

7 3 5 816.72 2.751216 NUl**

2 0 2 70 . 08 0.013376 2NU2

6 2 4 602 .77 2.751216 2NU2

5 2 3 446. 50 0.386397 NUl

5 3 3 2126.41 2. 324407 NU1**^<-

9 2 7 2818 .40 3. 529968 NUl***

6 4 2 757. 78 0.084732 NUl

7 3 5 816.72 2.751216 NUl

10 3 7 1538.23 2.171641 NUl

13 1 12 2042.33 3. 76133 2NU2

6 3 3 661 . 56 0.051901 NUl

11 2 10 1525.13 1.851690 NUl

9 2 7 1201 .95 3. 529968 NUl*

11 1 10 1524.87 1.851910 NUl

7 3 4 842 .38 0.214427 NU3*

8 4 4 1131 .76 4.012859 2NU2

3 3 0 1907.63 3.393148 2NU2***

3 3 1 1907.47 3. 390390 2NU2***

9 6 3 1631.41 0.059724 NU3

11 4 7 1899.06 37.2 NU1 +

12 3 10 1962.55 3.648229 NUl

13 2 12 2042 .38 3.75319 2NU2

5 4 1 610.35 0.031887 NUl*

13 2 11 2246.98 11.888730 NU3

14 1 13 2327.88 13.271580 NU3

14 2 13 2 32 7.90 13.271150 NU3

5 3 2 508.81 1.841317 NUl*

27
LINE HALF

FREQUENCY STRENGTH WIDTH J' K J" Ka '^c E" L BAND

cm > Cff)—

1

gm cm~ ^ U 1 1 M. 3437.12 0.0073 0.0552 8 1 7 9 2 8 1080.38 6.019178 NU 1*

3437. 38 0.0017 0.0752 10 3 7 1

1

3 8 3441 , 09 9. 899853 NU3***

3437 , 1 .0818 0.0704 7 5 2 7 4 3 931,22 3 . 03927

1

2NU2

3437.42 0 ,6686 0.0536 10 4 1

1

5 2 144 , 12 7 . 774282 NU3

3437 . 76 0 .4621 0.0658 1

1

3 8 1 2 3 9 2105 • 90 1 0 . 74443 5 NU3

3438.02 0.0014 0.0430 9 7 3 1

0

7 4 2054, 40 5. 133658 NU3*

3438 . 03 0.0013 0.0834 8 3 6 9 2 7 1201,95 3 . 529968 NUl**

3438.07 0.0397 0.0681 8 1 8 8 'X X w W • X n. 005795 NU3

3438 . 08 0.2229 0.0515 10 6 5 1

1

2 142 , 69 7. 773013 NU3

3438.18 2.8088 0.0824 5 2 3 6 4 2 757.78 0.086601 NU3

3438.28 0.0295 0.0391 1 2 1 1

1

1 2 2 1X 0w 1960 .22 3.652921 NU 1 3438-5 0 0.9018 0.0548 1 1 X J. 4 8 1X 2C 4 9 7124.98 in. XVJ^^tJ 48 1399 X-/ y 7 NU3

3438 . 58 0.0277 0.0388 9 0 9 1X 0w 1X 10X w 1X 114.56 X X ^ • ^ \J 9.013676 NU 1*

3438.62 0.0092 0.0382 9 1 9 1 0 0 10 1114.55 9.013420 NU 1*

3438 . 64 0.2102 0.0320 14 1 14 1 5 1 15 2358 .44 14, 743490 NU3

3438 . 64 0.6306 0.0320 14 0 14 1 5 0 15 2358 .44 NU3

3438.74 0.1561 0.0703 6 0 6 6 4 3 756.75 0 . 00 1 595 NU3

3439. 18 0.0074 0.0432 13 3 1

1

1 3 4 10 2426 .22 5.48699 NUl

3439 . 20 0.6086 0.0787 5 1 4 5 4 1 610.35 0.031887 NU 1 3439.50 0.0216 0.0871 4 2 3 5 3 2 508.8 1 1X .841317 • vj X X 1 NU l-t^* 3439 • 5

1

0.0067 0.0465 6 1

1

7 5 2321,89 4. 990193 NU 1 3439.66 0.5908 0. 0646 5 1 5 4 2 757 , 78 2.089996 2NU2

3439.68 0.0702 0.0777 4 1 3 4 4 0 488,13 0.00 \y 9 \J \^ 5 990 y y \y NU 1 3439.81 0.0440 0.0592 8 4 5 8 5 2 1411 .68 0.035676 NU3

3439.82 0.0520 0.0374 9 8 1 1

0

8 2 2254,34 3.624262 NU3

3439 . 82 0. 1560 0.0373 9 8 2 1 0 8 3 2254, 34 3.624262 NU3

3439 . 96 2.3745 0.0779 4 2 3 5 4 2 610,12 0. 034972 NU3

3440 .08 0.0220 0.0646 8 2 7 9 1 8 1079,07 5 . 987889 NU 1*

3440 .13 1.9517 0.0580 5 5 0 5 4 1 610.35 1.101100 2NU2

3440 .21 0.0202 0.0497 1

1

6 5 1

1

7 4 2321 .94 4.999181 NU 1 3440 .36 0.6512 0.0566 5 5 1 5 4 2 610.12 1J- .9 100600 yy \y \^ \j \y 2NU2

3440 .58 1 .7783 0,0607 5 5 2 5 4 3 756,75 2.085226 2NU2

3440 .65 0,4327 0.0895 2 0 2 3 3 1 285,23 0.013376 NUl

3440 .75 0.3642 0.0624 7 5 3 7 4 4 927.77 3.012848 2NU 2

3440 .94 0 .0016 0.0875 5 0 5 A 7C 4 7 211 .71 0.069891 NU3***

3441 .31 0.0051 0.0869 \j X1 7 'X 4 842 .38 0.71 4477 NU3**

3441 . 62 0.0774 0.0852 5 2 3 5 3 4 648 .97 2.4525 23 NU 1*

3441 .77 0.0080 0,0653 7 1 6 8 2 7 2495 , 18 4.T w 996649 y y \^ T y NUl***

3441 .87 0.0051 0,0388 9 0 9 10 1 1 0 1114.56 9.013676 NUl**

3441 . 87 0.0556 0,0350 12 1 1

1

1

1

2 10 1525,13 9 .076485 2NU2

3441 . 91 0.0017 0.0382 9 1 9 10 0 10 1114.55 9. 013420 NU 1**

3441 . 97 0,0797 0.0680 3 3 1 4 4 0 488 .13 3.390390 NUl*

_? M" <1 . w 1 3 , 5091 0.0834 ao

•5D AD 9 c. 7 17m .95 ^» y C y y \J \J NUl

^44? _j ^ ^ t. .. J.1 5 0 .2393 0.0683 -3 n A 1X 488.10 3.^93148 NUl*

3447 ,77 2 .4484 0.0832 8 3 6 7 7 5 782 . 40 3.262769 2NU2

3442 .38 0.5343 0.0620 8 5 4 8 4 5 1122.72 3.901175 2NU2

344? .5? 58.4557 0.0871 A 7 3 15 2 508.81 1.841317 NU 1 3442 .71 0.1669 0.0350 1

2

2 1

1

1

1

1X X10>^ 1524.87 9 . 078065 2NU2

3442 .73 0.0164 0.0484 10 6 4 10 7 3 2054.40 4.061130 NUl

3442 • 76 0.1726 0,0578 7 4 4 7 6 1 1216 .20 0.017491 NU3

3443 .07 0.0143 0.0858 3 7 2 4 3 \ 2005.92 2 . 164905

3443 .10 1.8952 0.0700 1 0 5 5 1

1

5 5 1999.02 8.798801 NU3

3443.47 0.0041 0.0646 8 2 7 9 1 8 1079.07 5.987889 NUl**

3443.47 3 ,6582 0,0552 8 1 7 9 2 8 1080.38 6,019176 NUl

28
FREQUENCY

LINE HALF

STRENGTH

cm 1 WIDTH

cm-1

J' Ka J" K a E" cm-i

L BAND

gm cm -2 aim.

3444.07 0.0044 0.0887 6 3 3 5 2 4 416.22 1.411171 2NU2*

3444. 18 0.0010 0.0625 7 4 3 8 1 8 744. 16 0.001069 2NU2

3444.22 0.0143 0.0852 5 2 3 6 3 4 648 .97 2.452523 NUl-)^*

3444. 52 0.0147 0.0680 3 3 1 4 4 0 488.13 3. 390390 NUl**

3444,64 0.0174 0.0795 4 2 2 5 4 1 610.35 0.042579 NU3^^

3444.70 0.0443 0.0683 3 3 0 4 4 1 488. 10 3. 393148 NUl**

3445.02 0.0441 0.0552 6 4 3 6 6 0 1045.07 0.005704 NU3

3445. 11 0.0729 0.0600 9 5 5 9 4 6 1340.89 4.736397 2NU2

3445. 17 13.8539 0.0388 9 0 9 10 1 10 1114.56 9.013676 NUl

3445.21 4.6179 0.0382 9 1 9 10 0 10 1114.55 9.013420 NUl

3445.61 0.0504 0.0463 9 6 4 9 7 3 1810.63 3. 116005 NUl

3445.73 0.1513 0.0467 9 6 3 9 7 2 1810.63 3. 116419 NUl

3445.79 0.0019 0.0915 4 3 2 3 0 3 136.77 0.051049 2NU2*

3446.29 0.1327 0.0568 6 4 2 6 6 1 1045 .07 0.005721 NU3

3446. 52 0.0614 0.0674 4 4 1 3 3 0 285 .43 3.393148 2NU2*

3446.83 38.6857 0.0852 5 2 3 6 3 4 648.97 2.452523 NUl

3446.87 11.0009 0.0646 8 2 7 9 1 8 1079.07 5.987889 NUl

3446.95 0.0583 0.0610 7 4 3 7 6 2 1216.20 0.017690 NU?

3447.08 39.8404 0.0680 3 3 1 4 4 0 488 .13 3.390390 NUl

3447.25 119.6379 0.0683 3 3 0 4 4 1 488. 10 3.393148 NUl

3447.66 0.0762 0.0563 10 5 6 10 4 7 1581 .34 5.482102 2NU2

3448.40 13.7101 0.0869 6 1 5 7 3 4 842.38 0.214427 NU3

3448.78 0.3040 0.0440 8 6 3 8 7 2 1590.74 2. 144879 NUl

3448.83 0.1013 0.0441 8 6 2 8 7 1 1590.74 2. 144937 NUl

3449.03 0.0015 0.0520 9 6 3 10 6 4 1875.53 6.440055 NU3*

3449.09 0.6291 0.0588 10 5 6 11 5 7 1985.83 8. 747542 NU3

3449.36 0.0036 0.0889 5 1 4 6 3 3 2282.59 0.202769 NU3***

3449.45 0.0013 0.0710 6 3 3 6 5 2 2552.85 0.077000 NU3***

3449,47 0.0045 0.0508 9 6 4 10 6 5 1875.00 6.439836 NU3*

3449.65 0.0024 0.0427 7 7 0 8 6 3 1411,65 0.074321 2NU2

3449.66 0.0442 0.0674 11 3 8 10 4 7 1581 .34 3,178818 2NU2

3449.71 0.0462 0.0851 3 2 1 4 3 2 2004,81 2.320352 NUl*-^*

3449.83 0.0021 0.0604 9 5 5 10 5 6 3383 .36 7,532122 NU3***

3449.87 0.0231 0.0459 13 2 11 13 3 10 2414.73 5,73353 NUl

3449.97 0.0023 0.0393 10 1 10 10 2 9 1293 .66 1 ,847651 NU1^«-

3450. 17 0.1377 0.0646 8 4 4 8 6 3 1411 .65 0,037084 NU3

3450.21 0.0032 0.0795 4 2 2 5 4 1 610.35 0,042579 NU3**

3450.70 0.0031 0.0447 8 0 8 9 1 9 2512 .43 6,81 NUl-«-**

3451. 10 0.0108 0.0443 8 1 8 9 0 9 2512 .36 8,007087 NU1**«-

3451.20 0,0218 0.0620 10 3 8 10 5 5 1724.72 0.084234 NU3

3451.24 0.0022 0.032 14 2 13 14 1 14 2073.66 1,90878 2NU2

3451.89 0.1422 0.0409 7 6 2 7 7 1 1394.86 1, 119792 NUl

3451.89 0.4266 0.0409 7 6 1 7 7 0 1394.86 1 ,119797 NUl

3452.08 0.0024 0.0879 7 3 4 6 2 5 2161.30 0,996364 2NU2***

3453.15 0.2218 0.0431 9 7 2 10 7 3 2054.40 5, 133660 NU3

3453. 15 0.6654 0.0430 9 7 3 10 7 4 2054.40 5,133658 NU3

3453.39 0.3689 0.0754 9 3 7 8 2 6 982.91 4,004942 2NU2

3453.81 0.0057 0.0948 3 1 3 4 2 2 1922 .92 0.610552 NU1^<-**

3453.88 0.0269 0.0531 12 5 8 12 6 7 2433.85 6.631337 NUl

3453.92 0.0114 0.0674 4 4 1 3 3 0 285.43 3.393148 2NU2**

3454. 13 0.0038 0.0665 4 4 0 3 3 1 285.23 3.390390 2NU2^<-*

3454. 51 0.0027 0.0759 7 2 6 8 1 7 2490.37 4.913532 NUl***

3455.74 0.0280 0.0665 9 4 5 9 6 4 1631.27 0.066893 NU3

3455.79 8.7020 0.0795 4 2 2 5 4 1 610.35 0.042579 NU3

29
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm"l cm 1 gm cm- 2 atm.

3456.25 2.0134 0.0810 10

3456.35 0.0039 0.0671 9

3456.57 0.0485 0.0653 7

3456.72 1. 1622 0.0393 10

3457. 15 0,0118 0.0757 3

3457. 18 0.0507 0.0865 4

3457.21 0.0030 0.0563 10

3457.28 0.0022 0.0634 6

3457.33 0.3901 0.0397 10

3457.46 0.1608 0.0658 9

3457. 50 2.2123 0.0887 6

3457.99 0.6239 0.0928 6

3458.02 0.0434 0.0467 12

3458. 15 0.0052 0.0764 6

3458.24 0.0061 0.0742 5 3458.36 0.0010 0.0650 8

3458.37 0.0099 0.0875 5 3458.60 0.9428 0.0475 11

3458.67 0.1033 0.0425 11

3458.70 0.7092 0.0338 12

3458.70 2.1229 0.0338 12

3458.72 2 .3526 0.0447 11

3458.84 0.0157 0.0549 11

3459.44 0,0182 0.0719 5

3459.59 0.0124 0. 0604 9

3459.69 0,0090 0.0653 7

3459.84 0,1591 0.0494 11

3459.88 0,0094 0.0865 4

3459.98 0. 1597 0.0554 10

3460. 19 0.0654 0.0443 8

3460.35 0.0082 0.0866 4

3460. 36 5.1431 0.0752 10

3460.58 0.5918 0.0320 13

3460.58 1 .7862 0.0320 13

3460.60 0.0014 0.0691 11

3461 .07 0.9720 0.0915 4

3461.26 0.0528 0.0332 13

3461. 32 30.7223 0.0674 4

3461.53 10.2433 0.0665 4

3461.65 1 .3626 0.0603 10

3461.70 0.0176 0.0331 13

3461 .94 0.0040 0.0843 5

3462.58 25,3423 0.0865 4

3462.82 24,2543 0.0653 7

3462.83 0,3113 0.0445 11

3462.90 0.0161 0.0759 7

3462.95 0.0021 0.0500 8

3462.98 0.0045 0.0648 9

3463. 19 0,0019 0.0887 8

3463. 50 0.0041 0.0757 3

3463.53 0.0121 0.0443 8

3464.24 0.0014 0.0616 7

3464.25 0.7443 0.0520 9

3464.25 0.0013 0.0407 8

K J" Ka '^c E L

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cm-1

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30
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm-1

gm cm -2

cm~i

atm.

3464 .25 0.0037 0.0408 8 7 1 3464 .66 2.2332 0.0 508 9 6 4

3465 .88 0 .1099 0.0354 8 8 1 3465 .88 0.3298 0 . 0 3 54 8 8 0

3465 .88 0.0018 0.0875 5 C 5 3466 . 04 0.0630 0,0751 5 0 5 3466 .05 0 .4584 0.0657 10 3 8

3466 . 09 0.0039 0 ,0585 8 2 7

3466 .12 1 .4345 0 , 0608 8 4 4

3466 . 33 0.0048 0,0898 7 3 5 3466 .62 0.0670 0. 0845 7 3 4

3466 .87 32 .7206 0 • 0443 8 1 8

3467 . 04 9.2767 0 ,0447 8 0 8

3467 .50 1 .9978 0,0843 5 0 5

3467 • 96 0.0267 0,0 534 12 4 9

3468 .28 0.0030 0.0530 8 1 8

3468 .60 5.8795 0.0757 3 2 2

3469 .14 0.0021 0.0680 7 4 3

3469 . 1

8

0 .02 1

1

0.0320 14 0 14

3469 . 20 0,0864 0.0858 3 2 2

3469 .20 0.0070 0.0320 14 1 14

3469 . 41 0,0121 0.0817 9 3 6

3469.49 0,1636 0 . 0834 5 4 1 3469.61 0,0025 0.0620 6 4 3

3469 . 94 8 , 0734 0.0759 7 2 6

3470 . 16 0,0122 0 .0742 5 4 2

3470 .50 3 ,0644 0.0824 9 4 5 3470.86 0,0270 0 • 0648 9 4 6

3471. 12 0,0771 0.0841 2 2 1 3471 . 2

1

0,0028 0.0578 5 4 1 3471 . 24 0,0191 0.0840 4 4 0

3471 . 62 0,2181 0 . 0645 9 3 7

3471 , 64 0,0365 0.0719 5 4 1 3471 .87 0,0229 0.0534 7 0 7

3471 . 89 1 ,9665 0.0671 9 5 4

3472 . 10 0,0160 0.0858 3 2 2

3472 .32 0 ,0076 0. 0542 7 1 7

3472 .56 0,0023 0.0451 9 1 9

3472 .83 0,0260 0.0830 2 2 0

3472 . 85 0,0267 0.0842 5 1 4

3473.09 0,0708 0.0800 6 4 2

3473 . 30 4, 1084 0.0866 4 1 4

3473 . 39 4,9709 0.0875 5 0 5

3^4.73 , 46 0 , 947

1

0.0887 8 4 5 3473 .69 0,0068 0,0459 9 0 9

3473.98 0,0343 0 . 0948 3 1 3

3474. 55 0,0314 0.0764 6 1 5

3474,73 6,2214 0.0604 9 5 5 3474, 78 2 ,0881 0.0757 3 2 1 3474.90 0 ,0056 0 . 0640 8 5 3

3474,96 0,0215 0. 0889 5 1 4

3474. 97 2,4177 0.0898 7 3 5 3475.01 43. 1955 0.0858 3 2 2

3475.63 0.0012 0.0739 7 1 7

J" Kq Kc E" L BAND

cm"'

9 7 2 1810.63 3. 579254 NU3*

10 6 5 1875 .00 6.439836 NU3

9 8 2 2009 .87 1.901685 NU3

9 8 1 2009.87 1.901685 NU3

6 2 4 602 .77 0.069891 NU3-;*-*

5 4 2 610.12 0.000921 NU3

9 2 7 1201.95 4.932263 2NU2

7 5 2 1059.85 0.001936 NUl

9 1 9 920.21 12.48 NU2 +

8 2 6 982.91 2.422109 NUl-«-

7 0 7 586.26 0.033256 2NU2

9 0 9 920.18 8.007087 NUl

9 1 9 920.21 6.81 NUl5 3 2 508.81 0 .062476 NUl

12 5 8 2275 .44 6. 558344 NUl

8 2 7 2495 . 18 1.833129 NUl^*^

4 4 1 488 .10 0.015552 NU3

7 5 2 2724.19 3.039271 NUl-^-^*

14 2 13 2327.90 0.488990 NU3

4 3 1 383.85 2. 164905 NUl*

14 1 13 2327,88 0.489010 NU3

10 3 7 1538.23 9.029655 NU3*

5 1 4 399 .46 0.031887 2NU2

6 5 2 2552.85 1. 56 NU1**^<-

8 1 7 882.93 4.913532 NUl

4 3 1 383.85 3. 270203 2NU2*

10 4 6 1616.51 6. 830000 NU3-

10 4 7 1581.34 8, 354292 NU3^«-

3 3 0 1907 .63 2.366160 NU1>-**

5 5 0 2406 . 15 0.826 NUl***

4 1 3 275.52 0.005990 2NU2

9 5 4 1477 .31 0.080993 NU3

4 3 2 382.52 3. 250024 2NU2*

8 1 8 2337.70 7.000291 NUl***

10 5 5 1724.72 7. 545052 NU3

4 3 1 383.85 2. 164905 NUl**

8 0 8 2337.53 6.998008 NUl***

9 2 8 1080.38 1.842036 NUl*

3 3 1 1907.47 2. 394805 NUl***

6 2 5 2161 .30 3. 129447 NUl***

6 1 5 542 .91 0.084732 2NU2

5 3 3 504 .00 0.035251 NU3

6 2 4 602.77 0.069891 NU3

9 3 6 1282.92 1.416234 NUl

9 1 8 1079.07 1.844131 NUl*

4 2 2 315.79 0.610552 NUl*

7 2 6 709.60 4.008107 NUl*

10 5 6 1718 .77 7,532122 NU3

4 4 0 488.13 0.016542 NU3

9 5 4 3141 .06 6.258032 NU3***

6 3

Q 661 .56 0.202769 NU3*

8 2 6 982.91 2.422109 NUl

4 3 1 383.85 2. 164905 NUl

7 3 4 842 .38 0.009220 NU3*
LINE HALF

J' K FREQUENCY STRENGTH WIDTH Kq

crn-i cm 1 cm~^

gm cm^ nU tm1 1 1 1.

"3,^.7^ -3 *+ / J » 771 1 0 no 1 R nU , 0^07 O O f QO -/ 3475.93 0,0043 n . 0496 8 3

3475 . 94 0.0128 0.0 500 8 5 2

0O .0541 . V M- X n . n A n ft 1X 0<^ 3476 . 44 0.0098 n . 0644 X1 ?c~ 5 7

3476 .67 0,2802 0,0851 3 2 1 3476 .74 0 .0022 0.0817 9 3 6

0.1 579 n . 0 5 5ft QJ 3477 .17 0.0013 0.0459 9 0 9

3477.2 7 0 . 049

1

n . 0629 X1 1X 5 5

3477 . 36 0,0063 0 . 0 948 3 1 3

3477 .36 0 ,4756 0.0583 9 5 4

3A77 . 43 0,0049 0.0477 6 5 2

3477 , 44 0,0016 0.0478 6 5 1 3477 .59 0 ,0022 0.0 742 5 4 2

3477.61 0 , 0058 0.0 764 5 1 5 3477.7 1 0.3601 n . 0 5 5ft 8 3

3477 .78 1 .0793 0 . 0 S4B 8 4

3477 . 79 0,0157 0.0898 4 1 3

3477.8 8 0,0714 n . 0 5? R 1X 1X 3 9

3478 .29 0.00 50 n . 0648 9 4 A\J 3478,67 0.0032 0.0666 9 2 7

3479 • 03 0.0067 0.0719 5 4 1 3479 ,06 0.0095 0. 0800 6 4 3

3479.37 0.6232 0 . 0407 8 7 2

3479 ,37 1.8697 0 . 0408 8 7 1 3479 ,38 1.1312 0.0451 9 1 9

3479 - 45 0.051

8

n . 0 8 5 1 3 2 X 3479 .58 0.6609 n . 0 5 1 ft 7 5 3

3479,60 1.9832 0.0521 7 5 2

2)^19 ,11 0 .0415 0.0 579 1

1

4 8

3480 , 22 1 .0608 0 . 0486 1X 0>^ 2 9

34R n . 3

1

\J W " w V u • w U U 1 1X 0\J 4 A

34fl0 .39 9 . 08 ? 5 1X 0w 2 8

3480 . 65 2.2914 0.0361 1

1

1 10

3480 .65 6.8739 0. 0360 1

1

2 10

3480 .66 3 .4212 0.0459 9 0 9

3480 .67 1 5 . 7 1 ?6 n . 0 764 A 5

3480 . 74 1X 7.1473 ' • X ~ 1 —0 . 094R 3 1 3

3480 .89 3,0124 0.0515 1X 0V 3 8

348 1 . 06 0,0118 0.0815 8 4 4

J " U i • 1 0.1 388 n - n 5 34 7 n 7

*T O X • 1 0.0073 vj . w *+ v-* ^ X1 0w X 9

-? " O X • ^ 0 . 04 A n . n S4P 7 TX 7

348 1.63 2 , i^i^i^^ 0 .0477 6 5 2

348 1 . 64 0.8149 0.0478 5 5 1 348 1.67 0 , 0040 0.0 889 5 1 4

3482 .24 140 ,1098 0.0851 3 2 1 3482 . 41 2,2189 0.0325 12 1 12

3482 • 41 6,6590 0.0325 12 0 12

34fl? .57 0.01 48 n . 0 3 3 1 4 2 1

3

0 00 1 ft n n A 7 R 7 c; 3483. 15 0,0031 0.0755 6 4 2

3483.53 0,0023 0.0500 8 6 2

i" J

1/Kq Kc P" L BAND

cm"'

9 5 5 3139. 50 6,255627 NU3***

9 6 4 1631 .27 5,032027 NU3*

9 6 3 1631.41 5,032058 NU3*

10 6 4 1875.53 4, 974368 NUl

12 6 6 2437,56 7,235377 NUl

4 3 2 382,52 2,320352 NUl^J10 3 7 1538,23 9, 029655 NU3**

9 6 4 1631,27 4,001691 NUl

9 1 8 1079,07 1,844131 NUl-J^*

1

1

6 5 2144,12 6,009423 NUl

4 2 2 315 ,79 0.610552 NUl**

9 6 3 1631,41 4,017231 NUl

6 6 1 1045 .07 1. 111607 NUl*

6 6 0 1045 . 07 1 . 11 1654 NU 1*

4 3 1 383.85 3.270203 2NU2**

7 2 6 709 , 60 4.008107 NUl**

8 6 2 1411 .68 3.077042 NUl

8 6 3 1411.65 3,073714 NUl

5 3 2 2130.50 0, 137702 NU3***

1

1

4 8 1843.02 5,243402 NUl

10 4 7 1581.34 8, 354292 NU3**

10 2 8 3058,41 9, 000870 NU3***

4 3 2 382,52 3. 250024 2NU2**

5 3 2 2130 , 50 3. 153879 2NU2***

9 7 3 1810,63 3.579253 NU3

9 7 2 1810.63 3. 579254 NU3

9 2 8 1080.38 1 .842036 NUl

4 3 2 382.52 2.320352 NUl**

7 6 2 1216.20 2. 119434 NUl

7 6 1 1216,20 2. 119964 NUl

1

1

5 7 1985,83 6.097371 NUl

10 3 8 1446, 16 3.605841 NUl

10 6 5 1875,00 0. 114652 NU3

1

1

2 9 1690.70 9.932549 NU3

12 1 11 1774.60 11.275820 NU3

12 2 11 1774.74 11 .275004 NU3

9 1 8 1079.07 1 , 844131 NUl

7 2 6 709.60 4,008107 NUl

4 2 2 315.79 0.610552 NUl

11 3 9 1695 .03 9.881611 NU3

9 4 5 2998 . 78 7. 302001 NU3***

8 1 8 744, 16 7.000291 NUl*

11 1 10 3135,82 10.283342 NU3***

8 0 8 74A,09 6.998008 NUl*

6 6 1 1045,07 1. 111607 NUl

6 6 0 1045 ,07 1. 111654 NUl

6 3 3 661 ,56 0. 202769 NU3**

4 3 2 382,52 2.320352 NUl

13 1 13 1806 ,78 12 . 744430 NU3

13 0 13 1806 ,78 12.739050 NU3

13 1 12 2042 ,33 9. 74091 2NU2

7 5 2 1059,85 0.041795 NU3*

5 3 3 2126,41 3.066224 2NU2***

9 6 3 163.1 ,41 5.032058 NU3**

32
LINE HALF

J" r" 1 BAND

FREQUENCY STRENGTH WIDTH J' Ka Kc Kq

gm cm~2 u Tin.

3484, 07 6,0352 0.0817 9 3 6 1 0 3 7 1538.23 9.029655 NU 3

3484 .12 0,1527 0.0756 7 4 3 7 1 6 704 . 22 0 , 13 5960 2NU2

3484. 40 0 ,0340 0. 0640 8 5 3 9 5 4 1477.31 6,258032 NU3*

3484. 73 0,0257 0. 0534 7 0 7 8 1 8 744. 16 7,000291 NUl**

3484 .93 0,0086 0,0542 7 1 7 8 0 8 744, 09 6 , 998008 NUl**

3485.03 6,0755 0,0742 5 4 2 4 3 1 383 .85 3,270203 2NU2

3485 . 1

1

0 , 1744 0.0669 8 3 6 8 5 3 1255 .92 0,064192 NU3

3485 . 48 0,0123 0.0687 6 1 6 5 4 1 610.35 0, 000636 NUl

3485 . 72 1 3 ,4802 0 .0648 9 4 6 10 4 7 1581 . 34 8, 354292 NU3

3485.92 0,0710 0.0815 8 4 4 9 4 5 1360 .28 7, 302001 NU3*

3486 • 06 0,0019 0.0870 0 4 4 3 1 383.85 0,047652 NUl-K3486 . 43 18 ,2424 0.0719 5 4 1 4 3 2 382.52 3,250024 2NU2

3486 . 52 0 ,1040 0.0770 4 0 4 4 4 1 488 . 10 0.000274 NU3

3486.71 0 .0037 0. 0547 1

1

6 5 12 5 8 2275 .44 0, 908981 NUl

3486 • 74 0.0138 0. 090

1

4 1 3 5 2 4 2024. 17 2,444582 NUl*^*-^

3486 . 97 0.0185 0.0424 12 2 10 1

1

3 9 1695 . 03 6 , 964699 2NU2

3487 .05 0 .0048 0.0879 7 3 4 6 2 5 552.92 0. 996364 2NU2*

3487 . 68 0.0197 0 .0666 9 2 7 10 2 8 1438 • 00 9. 000870 NU3*

3487.78 0,3733 0.0520 10 1 9 10 2 8 1438 .00 3.646815 NUl

3487 .82 0,0922 0.0848 6 2 5 7 1 6 704.22 3. 799063 NUl*

3488.09 69,4023 0,0534 7 0 7 8 1 8 744. 16 7.000291 NUl

3488.31 23,1376 0,0542 7 1 7 8 0 8 744,09 6,998008 NUl

3488 . 38 10, 7964 0,0889 5 1 4 6 3 3 661,56 0, 202769 NU3

3488 . 74 0,0044 0 ,0469 7 6 2 8 6 3 3101.19 3,52 2863 NU3***

3489. 03 0,4267 0.0613 10 4 7 10 5 6 1718 .77 5,482102 NUl

3489. 11 0,0056 0.0658 1

1

4 7 1

1

6 6 2142.69 0, 195288 NU3

3489 . 33 0 ,0026 0.0715 5 1 5 4 4 0 488 . 13 0,000220 NUl

3i^89 » 46 0,0012 0.0613 9 1 8 9 2 7 28 18 . 40 3, 674255 NUl***

3489. 56 0,0191 0.0864 8 3 5 9 3 6 2904.69 8 , 066869 NU3***

3490,29 0 ,0020 0,0380 7 7 0 8 7 1 1590 . 74 1 ,887603 NU3*

3490.29 0,0058 0,0380 7 7 1 8 7 2 1590.74 1 ,887603 NU3*

3490. 54 0 , 5967 0,0739 7 1 7 7 3 4 842 . 38 0, 009220 NU3

3490, 55 0,1619 0,0842 5 1 4 6 2 5 552.92 3, 129447 NUl*

3491 , 10 2 .1246 0, 0496 8 6 3 9 6 4 1631.27 5,032027 NU3

3491 , 13 0,9552 0, 0870 4 0 4 4 3 1 383.85 0, 047652 NUl

3491 , 1

3

6,3739 0,0500 8 6 2 9 6 3 1631 .41 5,032058 NU3

3491 ,49 0,0171 0.0848 6 2 5 7 1 6 704.22 3, 799063 NUl**

3491 .63 0,0189 0,0800 6 4 3 5 3 2 508 .81 3 , 153879 2NU2*

3491 ,78 0,1073 0.0814 9 5 5 10 4 6 1616.51 2,53 NUlH3491 .82 0 ,0079 0 .0648 5 3 3 5 5 0 742 . 10 0,037100 NU3*

3491.86 0.0283 0 .0327 13 0 13 13 2 12 2042 . 38 0, 486060 NU3

3491 .91 0 .0849 0,0327 13 1 13 13 1 12 2042 .33 0,4861 10 NU3

3492. 06 0.0063 0,0640 8 5 3 9 5 4 1477 .31 6,258032 NU3**

3492 . 34 0,0145 0 ,0647 6 0 6 7 1 7 2181.12 5,990506 NUl***

3493 . 42 0,9133 0,0675 7 3 5 7 5 2 1059.85 0, 041795 NU3

3493 . 44 0,0021 0,0607 8 5 4 9 5 5 1474 ,99 6,255627 NU3**

3493 . 59 0 ,0299 0.0842 5 1 4 6 2 5 552 .92 3 , 129447 NUl**

3493 .65 0 ,0434 0.0671 6 1 6 7 0 7 2180.65 5,983681 NUl***

3493 .73 0,0131 0.0815 8 4 4 9 4 5 1360 .28 7,302001 NU3**

3493 .83 0,0016 0 .0732 7 3 5 7 4 4 2569 ,52 3, 637027 NUl***

3493 , 96 0,0022 0. 0563 9 2 8 9 3 7 1216,27 3 , 554957 NUl*

3494. 1

1

0 ,0010 0.0420 12 1 12 1

1

2 9 1690 , 70 0,011432 NUl

3494.14 0,2294 0.0692 8 2 7 8 4 4 1131 ,76 0,045112 NU3

3494,42 0.1161 0.0864 8 3 5 9 3 6 1282,92 8,066869 NU3*

33
LINE HALF

FREQUENCY STRENGTH WIDTH J' J" Kc E" L BAND

cm 1 cm-'

gm cm -2

cm-1

atm.

cm-'

57 0.0180 0,0530 8 1 8 8 2 7 8 8 5,62 1,833129 NU l-*<- 3494 ,80 0.7668 0,0 590 1 0 3 8 1 0 4 7 1581,34 5,051335 NU 1 3495 , 1

6

46.0968 0,0848 6 2 5 7 1 6 704.22 3,799063 NU 1 3495 • 50 0,0104 0,0 594 9 3 7 1

0

3 8 1 446 .16 8,878817 NU 3*-**- 3495 .60 0.0260 0.0682 8 4 5 9 4 6 1 340 .89 7,216366 NU3^'<- 3495 .93 0,0031 C . 0666 5 3 2 5 5 1 742 .10 0.043 3 00 NU3*

3496 . 1 7 0 ,0437 0.0950 2 1 2 3 2 1 1819.34 0,92 528 2 NU 1*-*^*

3496 .41 0,0056 0.0616 1

1

5 6 1 2 4 9 2124.98 0,678814 NU 1 3496 .41 0 ,4083 0 .0639 9 4 6 9 5 5 1474, 99 4, 736397 NU 1 3496.63 80 ,9344 0. 0842 5 1 4 6 ^ 2 5 552 .92 3 , 129447 NUl

3497 . 02 0,0015 0.0648 5 3 3 5 5 0 742.10 0,037100 NU3**

3497 . 3

1

0,00 6 3 0.0755 6 4 2 5 3 3 504 . 00 3,0662 24 2NU2*

3497 .41 0 ,40 10 0.0880 5 3 3 4 0 4 222.06 0,095779 2NU2

3497 . 55 0 , 4671 0. 0841 2 2 1 3 3 0 285.43 2.366160 NUl*

3497 .81 0% 00 1 7 0.0 762 5 2 4 5 4 1 2251 . 86 0.024136 NU3*-s<-*

3497 .97 0,0164 0.0661 1 0 6 5 1

1

5 6 1999.02 0. 799607 NUl

3498 .00 0,0033 0.0530 8 1 8 8 2 7 885.62 1 .833129 NU 1**

3498 .59 0,3673 0.0665 6 3 4 6 5 1 888.63 0.021403 NU3

3498.8 5 0,0011 0.06 50 8 4 5 8 5 4 1255 . 16 3.901175 NU 1**

3499.06 0,1578 0.0830 2 2 0 3 3 1 285.23 2. 394805 NUl*

3499 .14 0,0035 0.0800 6 4 3 5 3 2 508.81 3. 153879 2NU2**

3499 . 34 0,0U90 0. 0739 6 3 4 6 4 3 2398 . 39 2 .878858 iMUl***

3499.41 0,0014 0 . 0834 7 4 4 6 3 3 2282.59 3.050978 2NU2***

3499 .65 0 ,0041 0.0645 7 4 4 7 5 3 1059.65 3 .012848 NUl*

3499 .73 16.9887 0.0640 8 5 3 9 5 4 1477.31 6.258032 NU3

3499. 96 2.3947 0.0879 7 3 4 6 2 5 552.92 0.996364 2NU2

3500. 23 0.0341 n . 0886 3 1 3 4 3 2 382.52 0.026225 NU3*

3500. 30 0.0561 0.0454 12 3 10 1 1 2 9 1690.70 7' .9 003088 Ni/ ^ \j V-* 2NU2

3500.33 0.0290 0.0760 8 2 6 9 2 7 28 18 . 40 8. 1 1347

1

NU3***

3500.37 0.0047 0.0885 3 1 2 4 3 1 2 005.92 0.066374 f\|U3***

3500.41 0.08 64 0.0841 2 2 1 3 3 0 285 ,43 2. 366160 NU I**

3500,65 0 ,0030 0.0482 1

1

7 4 1 2 6 7 2433,85 0, 724220 NUl

3500. 80 1 .1104 0.0563 9 2 8 9 3 7 1216 ,27 3, 554957 NUl

3501.02 5 .7541 0.0607 8 5 4 9 5 5 1474,99 6,255627 NU3

3501.22 3 .0147 0.0650 8 4 5 8 5 4 1255,16 3,901175 NUl

3501.33 0 . 0045 0.0608 7 5 2 8 5 3 2920.16 4, 904299 NU3***

3501 . 43 8.9974 0,0530 8 1 8 8 2 7 885.62 1,833129 NUl

3501.54 3 5.5074 0,0815 8 4 4 9 4 5 1360.28 7,302001 NU3

3501 .61 0.0600 0,0930 3 1 2 4 2 3 1907.99 1 . 970843 NU I***

3501.76 9 .6584 0.0 666 9 2 7 1

0

2 8 1438 . 00 9.000870 NU3

3501 .90 0,0292 0,0830 2 2 0 3 3 1 2.394805 NU I**

3501.94 0,0215 0,0 864 8 3 5 9 3 6 1282 .92 8.066869 NU3**

3502 . 04 0,0876 0 .0647 6 0 6 7 1 7 586.48 5.990506 NUl*

3502.22 0,0089 0 . 0469 7 1 8 5 2 1411.68- 3 . 522866 NU3*

3502 .22 3,9765 0.0648 5 3 3 5 5 0 742 , 10 0.037100 NU3 + 3502.2 5 0,0266 0,0469 7 6 2 8 6 3 1411,65 3. 522863 NU3*

3502.38 22 ,0795 0 . O4O2 10 1 9 1

1

1 10 1524,87 10.283342 NU3

3502 . 40 7,3583 0.0397 10 2 9 1

1

2 1 0 1525 ,13 10.281117 NU3

3502.70 0,2630 0.0671 6 1 6 7 0 7 586,26 5.983681 NUl*

3502.77 28,0151 0,0 594 9 3 7 1 0 3 8 1446 ,16 8 .878817 NU3

3503.28 233 , 5445 0,0841 2 2 1 3 3 0 285 ,43 2. 366160 NUl

3 5 03.40 0.4777 0,0757 8 4 4 8 X. 7 882,93 3.07 2NU2 + 3503.48 0,2785 0.0614 11 2 9 11 3 8 1813,26 5.642326 NUl

3504. 12 7,0357 0.0335 11 0 11 12 0 12 1557,91 11.742873 NU3
LINE HALF

Kq FREQUENCY STRENGTH WIDTH J'

4 cm ' cm""'

o gm cm ^

n m— 1 L-i 1

1

0 tm.

3504, 12 21.1072 0.0335 11 1 11

3504. 30 2 .0659 0.0645 7 4 4

3504.32 2 .5886 0.0548 8 0 8

3504.74 78.9022 0.0830 2 2 0

3505.37 0.0129 0.0699 4 3 2

3505.42 0.9658 0.0380 7 7 0

3505.42 2.8974 0.0380 7 7 1 3505.43 0.0162 0.0647 6 0 6

3505.52 0.0838 0.0 901 4 1 3

3505.89 7,5510 0.0620 6 4 3

3505.92 1.6510 0.0874 3 0 3

3506.08 1 ,5485 0.0666 5 3 2

3506.09 0.0953 0.0898 4 1 3

3506. 13 0.0486 0.0671 6 1 6

3506.65 9 .4693 0.0800 6 4 3

3507.75 0.0205 0.0354 10 0 10

3508.17 0.0125 0.0680 7 4 3

3508.55 0.0155 0.0901 4 1 3

3508.81 0,1759 0.0760 8 2 6

3508.82 43,8189 0.0647 6 0 6

3509.01 0.7997 0.0651 9 3 7

3509. 04 0.0179 0.0889 7 3 4

3509.46 0.0080 0.0920 5 2 4

3509.46 58 .0876 0.0864 8 3 5

3509,57 131 .4829 0.0671 6 1 6

3510.07 0 .0473 0.0674 8 3 6

3510.50 12 .4713 0.0927 6 3 4

3510.60 12.9950 0.0682 8 4 5

3511,59 41.9220 0.0901 4 1 3

3512.00 3.1481 0.0755 6 4 2

3512.04 0.0727 0.0771 5 0 5

3512.32 0.0813 0.0594 7 5 3

3512.54 0.0176 0.0898 4 1 3

3512.57 6,2667 0.0680 7 4 3

3513.00 0,0154 0.0743 6 1 6

3513.03 17.0244 0.0886 3 1 3

3513.11 0.0320 0.0701 7 4 4

3513.13 0.0187 0.0646 8 2 7

3513. 18 0.8767 0.0715 8 4 4

3513.27 0,0954 0.0587 9 6 3

3513.30 3,3793 0.0637 6 4 2

3513.38 0,0914 0.0928 4 0 4

3513.45 0,0174 0.0378 13 2 11

3513.80 0,6475 0.0894 7 4 4

3514.08 3,7290 0.0613 9 1 8

3514.12 8,3355 0.0578 5 4 1 3514.19 0,0488 0.0920 5 2 4

3514.45 0,3000 0.0337 12 0 12

3514.59 0,1000 0.0337 12 1 12

3514,87 0,0242 0.0806 5 1 5

3515.53 0,0129 0.0705 8 3 6

3515.63 2,5912 0. 0574 5 4 2

3515.89 0,0621 0.0787 7 4 3

3515.94 0.0144 0.0634 7 1 7

1" E" L BAND

cm"'

1 <i 1 12 15 5 7,91 ll,7«4-2858 NU3

7 5 3 10 59,65 3,012848 NU 1

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3 3 1 2 . 394805 Mill NU 1

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5 3 2 508.81 0. 137702 NU 3^

7 0 7 586.26 5,983681 NU I**

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-7 1 ( 5 86. 48 5,990506 NU 1 4 6 1340 .89 4, M4D21 NU 1 8 3 5 2670.79 6,985053

0 1 5 2 146 .28 2,6 /178o NU 1***

y 3 6 1 <i 82 . 92 8,066869 Ml 10 NU3

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-71 386.26 3 , 983681 M 1 1 1 NU 1 3 7 1216.2

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1 5 2 1059 .85 3.039271 Mill NU 1 6 2 5 2161.30 1 . 783035

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6 5 1 8 8 8 .63 2 . 089996 Mill NU 1 5 2 3 446 .50 0.096503 Ml 10^ NU 3*

1 2 3 1

0

1962.55 7.82232 0 M 1 10 2NU2

8 3 5 1050.15 0.898681 M 1 1 1 NU 1 0 I 1^01 .95 3.6 f4255 M t 1 1 c c:

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D 1 O ^ "7 1 "7 Q Q Z »tl 1 1. / 88 IN U i. *

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5 5 1 742 ,10 0.77 NU 1-

8 4 4 1131.76 6.039574 NU3*

7 2 6 709 ,60 1.816721 NUl*

35
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm-' cm ' cm 1 gm cm -2 atm.

3515.95 0.0326 0. '^Ib^ 8 2 6

3516.05 0.0128 0.0352 13 1 12

3516. 19 0.2649 0,0950 2 1 2 3516.23 0.0358 0,0529 1 0 6 5

3516 .87 0.0235 0.0456 9 2 8

3517. 01 0.C322 0,0534 9 6 4

3517.25 0.0386 0.0359 13 2 12

3517.37 4,4441 0 .0469 7 6 1 3517.40 13.3324 0. 0469 7 6 2

3518.17 0.0272 0.0959 2 1 1 3518. 50 0.6071 0 .0466 6 6 1 3518.65 0 .4065 0,0515 7 6 1 3518.71 0.0159 0.0783 6 2 5

3518.72 0.1671 0,0469 6 6 0

3518.85 0.1355 0,0506 7 6 2

3518.99 47.6211 0 ,0898 4 1 3

3519.04 1 .3098 0,0740 9 4 5

3519.22 0.3765 0.0527 8 6 3

3519.45 3 .9872 0.0710 6 3 3

3519.46 0 .0490 0. 0950 2 1 2

3519.46 0.2229 0.0553 8 6 2

3519.82 9.3408 0.0646 8 2 7

3519.91 0.0151 0.0594 7

'-) 3

3520.26 0,7478 0.0858 7 2 5 3520.70 0 .0450 0.0656 7 0 7

3520.75 0.0169 0.0928 4 0 4

3520.89 0.3635 0,0 930 1 2

3521 . 13 0 . 1942 0, 0701 7 4 4

3521. 16 2 .0392 0.0727 7 2 6

3521.30 6 .4342 0.0705 8 3 6

3521.35 0.0227 0.0675 12 3 9

3521 .43 0. 1079 0.0889 7 3 4

3521 .94 24.3889 0.0920 5 2 4

3522.27 0 .4409 0.0771 5 0 5 3522.73 132 .4740 0.0950 2 1 2

3522.80 7.2081 0.0634 7 1 7

3523 .10 87 .9754 0.0760 8 2 6

3523.64 0.0115 0. 0787 7 4 3

3523.77 0 . 1468 0.0 806 5 1 5 3523.93 0.0552 0.0559 8 1 7

3523 .97 0 ,0673 0.0930 3 1 2

3523 .98 2 1 ,3062 0.0467 9 1 8

3524.08 63 ,4693 0.0456 9 2 8

3524.53 0.0182 0.0535 8 2 7

3524. 76 23 .6949 0.0674 8 3 6

3524. 90 1 .4301 0.0834 7 4 4

3525.20 0.0131 0. 0738 12 4 8

3525.23 0 . 1605 0 .0755 10 4 6

3525.57 0 . 1664 0.0755 1

1

4 7

3525 .60 20.6930 0.0354 10 1 10

3525.60 62 .0796 0.0354 10 0 10

3525.67 0.0816 0.0771 5 0 5 3526.31 0.0553 0.0736 7 3 5 3526.99 13.4895 0.0608 7 5 2

J" Kc E" L BAND

cm-1

9 2 7 1201 .95 8. 113471 NU3**

13 3 11 2248.16 0.878880 NU3

3 2 1 212.15 0.925282 NU1^<-

10 5 6 1718.77 4.913223 2NU2

10 2 9 1293.66 9.287364 NU3**

9 5 5 1474.99 4.001691 2NU2

13 2 11 2246 .98 0.881500 NU3

8 6 2 1411.68 3. 522866 NU3

8 6 3 1411.65 3.522863 NU3

3 2 2 1813.81 1.666667 NUl***

6 5 2 888.60 1.346 2NU2 +

7 5 2 1059.85 2. 119964 2NU2

6 3 4 2271 .70 2.963539 NUl***

6 5 1 888 .63 1, 111654 2NU2

7 5 3 1059.65 2. 119434 2NU2

5 3 2 508 .81 0. 137702 NU3

9 5 4 1477.31 5.113359 NUl

8 5 4 1255. 16 5.22 2NU2 +

6 5 2 888 .60 0.077000 NU3 +

3 2 1 212.15 0.925282 NUl**

8 5 3 1255.92 9.32 2NU2 +

8 3 6 1006.12 3.456295 NUl

8 5 4 1255.16 4.903948 NU3**

6 1 6 447.24 0.182385 2NU2

7 1 (S 704.22 1.838288 NUl*

5 2 3 446.50 0.096503 NU3**

4 2 3 300.35 1.970843 NUl*

8 4 5 1122.72 6.014663 NU3*

7 4 3 931.22 0.048724 NU3

8 4 5 1122 .72 4.264036 NUl

12 4 8 2205.65 8.242761 NUl

8 3 5 1050. 15 6.985053 NU3*

6 1 5 542.91 2.671788 NUl

6 1 6 447.24 4.979001 NUl*

3 2 1 212.15 0,925282 NUl

7 2 6 709.60 1,816721 NUl

9 2 7 1201 .95 8, 113471 NU3

8 4 4 1131.76 6, 039574 NU3**

6 0 6 446 .71 4,958549 NUl*

9 1 8 2688.10 8, 308658 NU3***

4 2 3 300.35 1,970843 NUl**

10 1 9 1293.04 9,293415 NU3

10 2 9 1293.66 9,287364 NU3

9 2 8 2690.64 8,292239 NU3***

9 3 7 1216.27 7,070000 NU3-

6 3 3 661.56 3,050978 2NU2

12 5 7 2300.80 9, 504415 NUl

10 5 5 1724.72 6,465380 NUl

11 5 6 1999.02 8, 041630 NUl

11 1 11 1327. 14 10,743553 NU3

11 0 11 1327. 14 10,743597 NU3

6 1 6 447.24 4,979001 NUl**

8 3 6 2630.21 5,770000 NU3***

8 5 3 1255.92 4,904299 NU3

36
LINE HALF

Ka ^ FREQUENCY STRENGTH WIDTH J- cm"!

1 cm"' cm 1 gm cm-2 atm.

3527,05 181 ,7682 0,0930 3 1 2

3527 .22 0 .3897 0 ,0740 7 3 4

3527.43 0.1104 0,0641 9 5 4

3527.51 40.6879 0.0594 7 5 3

3528.03 22.5150 0,0656 7 0 7

3528.12 45.6895 0,0928 0

3528 .49 0.0127 0 ,0430 6 6 1 3528 . 49 0.0380 0.0430 6 6 0

3528.68 0 .0359 0 . 070

1

7 4 4

3529.07 220 .4414 0,0771 5 0 5 3529 . 15 3.3984 0 . 0794 8 5

3529.67 0,015 3 0.0722 7 2 6

3530.11 4.8586 0.0732 7 3 5

3530.33 0.0288 0.0885 3 1 2

3530.48 0 .1574 0.0838 7 2 5 3530.75 73 . 40 53 0,0 806 5 1 5 3530.77 0.3757 0,0701 1 0 2 8

3530 . 8

1

0.3347 0.0559 8 1 7

3530.98 0.1106 0.0535 8 2 7

3531.39 31 .0420 0,0787 7 4 3

3532,29 0 .3349 0,0736 7 3 5

3532.33 0.1096 0,0388 9 0 9

3532.34 0.3287 0,0388 9 1 9

3532.79 0 .0204 0,0758 9 4 5

3533 . 48 0.0101 0, 0739 6 3 4

3534. 28 0 .7996 0.0789 6 1 6

3534,99 0,0265 0 • 0737 5 3 3

3536.05 0 ,0934 0 .0743 6 1 6

3536. 15 7,6330 0. 0722 7 2 6

3536 . 15 27,1780 0,0739 6 3 4

3536.24 97,1271 0,0701 7 4 4

3536.57 0.1058 0,0914 4 1 3536 ,72 53 ,9853 0.0889 7 3 4

3536.90 0 , 3492 0,03 58 1

1

0 1

1

3537,16 1 ,0479 0.0359 1

1

1 1

1

3537.21 0,0662 0. 0748 6 4 2

3537,22 0,8921 0.0742 8 3 5 3537,34 0.1055 0,0993 1 1 0

3537,48 0,0171 0.0711 7 2 5

3537.53 0,0785 0 • 0699 3 2

3537.59 0 .0455 0.0 555 9 6 3

3537.78 0.0291 0.0838 7 2 5

3537 ,89 0 . 1648 0.0959 2 1 1 3538.01 0,0619 0.0 559 8 1 7

3538,25 0.0205 0.0535 8 2 7

3538,37 0,0118 0.0925 5 3 3

3538 .48 0,1933 0.0381 12 1 1

1

3538.54 0.1534 0.0 569 6 5 1 3538.59 0.0263 0. 0705 4 3 1 3538.61 0.0813 0 . 0759 5 3 2

3538.69 0.0164 0,0423 1 3 2 1

1

3538.71 0.0225 0.0 700 4 3

3538,71 0,0511 0.0565 6 5 2

3538,79 1 ,3423 0,0755 6 2 5

ill J Ka "^c b

1L RAND

4 2 3 300.35 1.970843 NUl

7 5 3 1059 .65 0.052981 NU3

10 4 7 1581 .34 0.720783 NUl

8 5 4 1255.16 4.903948 NU3

7 1 6 704. 22 1.838288 NUl

5 2 3 446 . 50 0.096503 NU3

7 6 2 1216.20 1.869458 NU3*

7 6 I 1216.20 1 . 869458 NU3*

8 4 5 1 122 . 72 6 .014663 NU3*7c

6 1 6 447.24 4.979001 NUl

9 4 5 1360.28 7.39 NU1 +

7 3 5 816.72 3 . 273499 NU 1*

7 4 4 927.77 3. 637027 NUl

4 3 1 383 .85 0.066374 NU3*

8 2 6 982 .91 7.251910 NU3*

6 0 6 446 .71 4.958549 NUl

10 3 7 1538.23 5.910419 NUl

9 1 8 1079 , 07 8.308658 NU3*

9 2 8 1080.38 8. 292239 NU3*

8 4 4 1131.76 6.039574 NU3

8 3 6 1006 . 12 5. 770000 NU3*

10 0 10 1114.55 9. 744485 NU3-«-

10 1 10 1 1 14. 56 9 . 744353 NU3^

9 1 8 1079 . 07 0. 116860 2NU2

6 4 3 756.75 2. 878858 NU l*-«- 6 3 3 661.56 0.014823 NU3

5 4 2 610.12 2.024051 NU 1*

6 2 5 552 .92 1.78303 5 NU 1-i^ 7 3 5 816.72 3 . 273499 NU 1 6 4 3 756.75 2.878858 NU 1 8 4 5 1122,72 6 .014663 NU3

5 0 5 1920 . 76 3.911752 MU l-i^^-«- 8 3 5 1050 .15 6.985053 NU3

1

1

2 10 1525.13 0.483142 NU3

1

1

1 1 0 1524.87 0.483240 NU3

7 4 3 2572.13 4.739627 NU3'*<'**

8 5 4 1255.16 0. 107233 NU3

2 2 1 1742 .28 1 . 500000 NU l-«--«-* 6 5 2 888 . 60 0.003511 NU 1 4 4 1 488 . 10 1 .082946 NU 1*

10 5 6 1718.77 0.576235 NU 1 8 2 6 982 .91 7.251910 NU3*^^

3 2 2 206.30 1

.

bbbbbl NU 1^<- 9 1 8 1079 . 07 8.308658 NU3''^-''*- 9 2 8 1080.38 8.292239 NU3**

6 2 4 602 . 77 0.863547 NU I*

1 2 3 1 0 1962 .55 0 . 873307 NU3

7 5 2 1059.85 3.450058 NU3*

4 4 0 488.13 1.088294 NU 1*

5 4 1 610.35 2 . 066632 NU l->*-

1 3 4 10 2426.22 1 . 1 1 2100 NU3

7 4 4 2569 .52 4.735129 NU3*^^^

7 5 3 1059.65 3.450020 NU3*

6 4 2 757. 78 0.040211 NU3

37
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm~' cm 1 cm 1 gm cm 2 Q tm.

3539 - 37 4-1621 0. 0774 7 4 3

3539.39 1.7280 0.0852 8 4 5

3539.43 0.0759 0.0885 6 3 3

3539.48 0,0173 0,0743 6 1 6

3539.57 0.0203 0,0388 9 0 9

3539.58 0.0608 0.0388 9 1 9

3539.60 0.9338 0.0804 6 3 4

3539.72 0,0620 0.0736 7 3 5 3539,95 0.2821 0.0755 1

1

3 8

3540 . 1 3 0.0145 0 .0699 4 3 2 3 540 .23 13.2722 0. 0737 5 3 3

3540.7 3 0,0306 0. 0947 2 3

3540 .86 0,0775 0,0391 1 2 2 1

1

3540 . 94 3,8376 0.0706 8 1 7

3541 . 02 0,0305 0.0959 2 1 1 3541.11 0,0150 0.0759 5 3 2

3541.51 0,2155 0.0880 4 0 4

3542 . 74 39,2409 0 .0699 4 3 2

3542.91 46,7236 0.0 743 6 1 6

3542 .99 14,3889 0.0885 3 1 2

3543.61 40,6415 0.0759 5 3 2

3543 ,64 6,3267 0.0430 6 6 1 3543 .64 18 .9800 0,0430 6 6 0

3543 .73 13. 1471 0.0705 4 3 1 3543 .81 0.1855 0 .0947 4 2 3

3544 . 1

5

82 .402

1

0.0959 2 1 1 3544, 17 0.0963 0.0783 6 2 5 3544 ,67 0 .0435 0.0670 7 1 6

3544, 79 0 . 40 1

1

0 .0748 6 4 2 3545 ,07 0 .6413 0.0914 4 1 4

3545 ,08 78.6951 0.0838 7 2 5 3545 ,21 167.3104 0.0 559 8 1 7

3545 ,52 5 5.2969 0.0535 8 2 7

3545 ,91 0.1282 0.0633 7 2 6

3546 ,13 0.02 83 0.0 569 6 5 1 3546 ,77 0.1872 0 .0894 6 2 4

3546 .82 54,7715 0.0388 9 0 9

3546 .83 164,3128 0.0388 9 1 9

3547 . 1

5

16 7 , 4662 0 .0736 7 3 5 3547 . 31 0,1916 0.0728 9 3 6

3547 . 58 5,8865 0.0925 5 3 3

3547 .84 0,0343 0.0947 4 2 3

3548 .05 0 ,1349 0.0952 3 0 3

3548 .33 4,6837 0.0873 2 1 2

3548 .34 10 7.7404 n . 0 880 4 0 4

3 548 .64 0,1186 0.0914 4 1 4

3549.03 0,0149 0.0 525 5 5 0

3549.14 0,0338 0. 0832 7 3 4

3549 .34 0 , 0484 0. 0907 4 1 4

3549. 57 0 . 1294 0 . 0447 8 0 8

3549 . 58 0,0431 0 .0446 8 1 8

3350 . 19 0.1228 0.0689 9 4 5 3550.22 0.4601 0.0885 6 3 3

3550.40 9 .6674 0.0801 6 3 3

J" Ka E" L BAND

cm~'

6 3 4 648.97 2. 767638 2NU2

7 3 4 842 .38 3.022183 2NU2

7 3 4 2462.87 3.480000 NU3***

6 2 5 552.92 1.783035 NUl**

10 0 10 1114.55 9. 744485 NU3**

10 1 10 1114.56 9. 744353 NU3**

5 0 5 325.35 0.123125 2NU2

8 3 6 1006. 12 5.770000 NU3**

11 4 7 1899.06 8.484859 NUl

4 4 1 488 . 10 1 .082946 NUl**

5 4 2 610.12 2.024051 NUl

5 1 4 2000.90 1.638916 NUl***

12 2 10 1960.22 0.875278 NU3

8 2 6 982.91 3. 773034 NUl

3 2 2 206.30 1 .666667 NUl**

5 4 1 610.35 2.066632 NUl**

5 1 5 326.64 3.972803 NUl*

4 4 1 488. 10 1.082946 NUl

6 2 5 552 .92 1.783035 NUl

4 3 1 383,85 0.066374 NU3

5 4 1 610,35 2.066632 NUl

7 6 2 1216,20 1.869458 NU3

7 6 1 1216,20 1.869458 NU3

4 4 0 488, 13 1.088294 NUl

5 1 4 399.46 1.638916 NUl*

3 2 2 206.30 1.666667 NUl

6 3 4 648 .97 2.963539 NUl*

8 1 7 2490.37 7, 336095 MU3***

7 4 3 931 .22 4, 739627 NU3*

5 0 5 325.35 3,911752 NUl*

8 2 6 982.91 7,251910 NU3

9 1 8 1079.07 8, 308658 NU3

9 2 8 1080.38 8,292239 NU3

8 2 7 2495, 18 7,292008 NU3***

7 5 2 1059,85 3,450058 NU3**

7 2 5 2392.58 6,352023 NU3***

10 0 10 1114.55 9, 744485 NU3

10 1 10 1114.56 9, 744353 NU3

8 3 6 1006.12 5,770000 NU3-

9 5 5 1474.99 0.205541 NU3

6 2 4 602 .77 0.863547 NUl

5 1 4 399.46 1.638916 NUl**

4 1 4 1821.61 3.004990 NUl***

3 3 1 285.23 0.013176 NU3

5 1 5 326.64 3,972803 NUl

5 0 5 325,35 3,911752 NUl**

4 4 1 2129,63 4, 396748 2NU2***

7 4 3 931.22 4, 268667 NUl*

4 2 3 1907.99 1.567300 NUl***

9 0 9 2512 .36 8. 745630 NU3***

9 1 9 2512.43 8.745235 NU3***

10 3 8 1446 . 16 0.409296 NUl

7 3 4 842.38 3.480000 NU3*

6 4 2 757.78 3,075987 NUl

38
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ~l

gm cm ~ 2 0 tm. 3550.41 48.1511 0.0783 6 2

3550.68 0.0521 0.0451 13 3

3550,72 0.1754 0.0947 1 1 3550.85 0.2124 0. 0844 9 4

3550.87 0.2555 0.0852 8 3

3551.24 0.0462 0.0885 2 1 3551.59 0.2640 0.0670 7 1 3551.87 92.7404 0.0947 4 2

3552.11 85.8435 0.0876 6 4

3552.11 0.7770 0.0633 7 2

3552.21 320.6569 0.0914 4 1 3552.39 17.0523 0.0777 6 0

3552.45 0.3525 0.0806 10 3

3552.83 2 .4224 0.0720 8 4

3553.42 0.7839 0.0447 8 0

3553.43 0.2613 0.0446 8 1 3553.44 1 .1343 0.0894 6 2

3553.45 0.0320 0.0516 5 5

3553.73 76.6965 0.0569 6 5

3553.86 16.9197 0.0832 7 3

3553.88 25.5662 0.0565 6 5

3554.49 0.0595 0.0839 5 1 3554.51 0.0134 0.0835 5 1 3554.74 0.0251 0.0700 6 4

3554.75 0.0380 0.0576 12 3

3554.77 0.0559 0.0833 5 2

3554.78 4.2757 0.0783 9 2

3554.85 0.3121 0.0694 10 3

3554.90 0.0118 0.0466 9 7

3554.92 0,0086 0.0650 10 4

3555.12 5 .0746 0.0762 5 2

3555.34 0,0541 0.032 13 1 3555.52 0.2283 0.0771 6 3

3555.68 0,0376 0.0884 5 2

3556.51 0,0122 0.0886 7 2

3557.14 87,7136 0.0947 1 1 3557.27 0,6393 0.0993 1 1 3557.48 0,2204 0.0801 10 4

3557.52 2 .7741 0.0844 8 3

3557.81 0.0103 0.0833 5 2

3557.83 0.0445 0.0647 11 3

3557.86 0.0110 0. 0839 5 1 3557.92 3.3222 0.0835 9 3

3557.94 0.0851 0.0885 6 3

3558.12 0.0667 0.0802 7 1 3558.29 0.0967 0.0477 12 2

3558.81 0.0488 0.0670 7 1 3559.08 3.2993 0.0393 10 0

3559.23 0.0431 0.0974 3 1 3559.43 0.1438 0.0633 7 2

3559.59 0.0283 0.0876 6 4

3559.69 0.8176 0.0952 3 0

3559.70 1 .1078 0.0397 10 1 3560. 14 200.5529 0.0748 6 4

Kc J" Kc E" L BAND

cm-1

5 6 3 4 648.97 2.963539 NUl

11 13 3 10 2414.73 1. 178730 NU3

1 2 2 0 136.17 1 .244747 NUl*

6 8 3 5 1050 . 15 3. 141455 2NU2

5 7 2 6 709.60 0.688192 2NU2

1 3 3 0 285.43 0.021579 NU3*

6 8 1 7 882 .93 7.336095 NU3*

3 5 1 4 399 .46 1.638916 NUl

3 7 3 4 842 . 38 13.89 NU1 +

6 8 2 7 885 .62 7. 292008 NU3*

4 5 0 5 325.35 3.911752 NUl

6 6 1 5 542 .91 1.852055 NUl

7 10 4 6 1616.51 8. 179783 NUl

4 9 3 7 1216.27 7. 64 NU1 +

8 9 0 9 920.18 8.745630 NU3*

8 9 1 9 920.21 8. 745235 NU3*

4 7 2 5 782 .40 6.352023 NU3*

1 6 5 2 2552,85 1.845180 NU3->^*-*

1 7 5 2 1059.85 3.450058 NU3

4 7 4 3 931 .22 4.268667 NUl

2 7 5 3 1059.65 3.450020 NU3

5 5 2 4 416.22 1.711792 NUl*

5 5 3 2 508 .81 0.019115 NU3*

3 7 4 4 927.77 4.735129 NU3**

9 12 5 8 2275 .44 0.855326 NU3

4 5 3 3 504.00 2.492169 NUl*

7 9 3 6 1282.92 6.247031 NUl

7 10 5 6 1718 ,77 0.369280 NU3

2 10 6 5 1875,00 0. 354752 NUl

6 11 3 9 1695, 03 0.293096 NUl

4 5 4 1 610.35 0.024136 NU3

13 14 0 14 2073 .66 12.99955 NUl

4 7 3 5 816.72 4. 550000 NU3*

3 5 3 2 2130.50 3.442901 NUl***

5 7 3 4 2462 .87 5. 91841

1

NUl***

1 2 2 0 136. 17 1.244747 NUl

0 2 2 1 134,91 1 , 500000 NU 1*

7 9 3 6 1282,92 3,465920 2NU2

5 8 4 4 1131.76 5, 709388 NUl

4 5 3 3 504.00 2,492169 NUl**

8 11 5 7 1985.83 0. 598994 NU3

5 5 2 4 416.22 1.711792 NUl**

6 9 4 5 1360.28 7.165263 NUl

3 7 3 4 842 .38 3.480000 NU3**

6 7 2 5 782.40 3.983004 NUl*

10 12 4 9 ,2124.98 1 ,085478 NU3

6 8 1 7 882,93 7,336095 NU3**

10 10 2 9 1293 ,66 0,478039 NU3

3 4 0 4 1817,50 2,831638 NUl***

6 8 2 7 885,62 7,292008 NU3**

3 7 3 4 2462 ,87 13,89 NUl***

3 4 1 4 224.83 3,004990 NUl*

10 10 1 9 1293.04 0,478334 NU3

2 7 4 3 931.22 4, 739627 NU3

39
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ' C(TI~1 cm~'

gm cm ^ otm.

3550, 22 0.2652 0 .0427 1

1

X X 1 3560 . 44 0.1183 0 . 0993 1 1 3560.68 0.0713 0.0952 3 0

3560.70 0 . 1450 0 , 0447 8 0

3560.72 0,0484 0,0446 8 1 3560. 85 27.9425 0.0833 5 2

3560.89 0 .2099 0. 0894 6 2

3561 . 24 29 »1105 0,0839 5 1 3561 .45 0,0726 0.0753 5 1 3561.95 1.1374 0.0750 4 2

3562.21 0,1019 0.0587 8 6

3562.32 68 .0243 0 .0700 5 4

3562.35 4.9576 0.0527 5 5

3562.38 14.8739 0.0525 5 5 3562.88 0.2288 0 .0845 4 2

3562 . 92 0.0214 0 .0944 3 1 3563 . 01 0.0423 0.0771 6 3

3563. 10 0.1513 0.0952 3 0

3563.61 319,6552 0.0993 1 1 3563.85 23 .0900 0.0885 2 1 3563.94 0.0374 0.0699 5 4

3564 .02 0.2162 0.0756 7 5 3564 . 45 0 . 0490 0 . 1006 2 0

3564.63 0.1129 0,0679 5 4

3564 .69 0.8018 0 ,0444 1

1

2

3564.72 46 . 4773 0. 0792 6 6

3564.92 0 .0647 0.0516 5 5 3564.95 0 . 1943 0.0516 5 5 3564.96 0.2798 0.0785 6 1 3565,67 230.0716 0.0885 6 3

3566.03 132.0104 0.0670 7 1 3566.04 33 .3505 0.0802 7 1 3 566 . 30 27.1083 0 • 0741 7 4

3566 .52 408.8145 0. 095? 3 0

3566.76 388.5256 J* V-/ W V w.* t_ ^ \J 0.0633 7 2

3567.17 0.2610 0 . 0974 3 1 3567 .23 0.0623 0. 0734 6 2

3567.45 0.0192 0 .0458 9 1 3567.99 391 .9608 0.0447 8 0

3568.01 130 . 6484 0 . 0446 8 1 3568.09 b ,1021 0.0835 5 1 3568,34 567.1561 0 . 0894 6 2

3568 .81 114. 3949 0.0845 4 2

3569.2 7 0.2179 0.0871 5 0

3569.61 0.5077 0 .0793 8 4

3570.06 0,0926 0.0535 7 0

3570.14 0,2779 0.0532 7 1 3570.50 114,1599 0.0771 6 3

3570. 55 0,2932 0.0907 4 1 3570.82 0 ,0483 0.0974 3 1 3571. 18 0,3481 0.0861 5 3

3571 .60 0,0158 0.0 598 6 5 3572.04 1.6961 0.0785 6 1 3572.15 0.1301 0.0917 5 2

J Kc t L DAIMU

cm-1

10 11 3 9 1695.03 0.850512 NU3

0 2 2 1 134.91 1 . 500000 NUl**

3 4 2 2 315.79 0. 116055 NU3*

8 9 0 9 920.18 8.745630 NU3**

8 9 1 9 920.21 8. 745235 NU3**

4 5 3 3 504.00 2.492169 NUl

4 7 2 5 782.40 6.352023 NU3**

5 5 2 4 416.22 1.711792 NUl

4 4 4 1 488.10 0.001994 NUl

3 4 4 0 488. 13 0.008789 NU3

3 9 5 4 1477.31 0.393126 NUl

3 7 4 4 927.77 4.735129 NU3

1 4 4 0 488 .13 4. 397010 2NU2

0 4 4 1 488 . 10 4.396748 2NU2

3 4 3 2 382.52 1.848533 NUl*

3 3 2 2 1813.81 1.297651 NUl-*^**

4 7 3 5 816.72 4. 550000 NU3**

3 4 1 4 224.83 3.004990 NUl**

0 2 2 1 134.91 1.500000 NUl

1 3 3 0 285.43 0.021579 NU3

1 6 4 2 2399.17 3.352166 NU3***

3 8 4 4 1131 .76 0.444062 NUl

2 3 1 3 1739.51 2. 156792 NUl***

2 6 4 3 2398.39 3.351648 NU3***

10 11 2 9 1690.70 0.856092 NU3

1 7 3 4 842.38 81.799998 2NU2 +

0 6 5 1 888.63 1 .845182 NU3*

1 6 5 2 888 .60 1.845180 NU3*

5 7 1 6 2309.74 6. 391209 NU3***

3 7 3 4 842 .38 3. 480000 NU3-

6 8 1 7 882.93 7. 336095 NU3

6 7 2 5 782 .40 3.983004 NUl

3 8 3 6 1006.12 9.90 NU1 +

3 4 1 4 224.83 3.004990 NUl

6 8 2 7 885.62 7.292008 NU3

3 4 0 4 222.06 2.831638 NUl*

5 7 2 6 2318 .53 4.390000 NU3***

9 9 1 8 1079.07 0.472318 NU3*

8 9 0 9 920. 18 8.745630 NU3

8 9 1 9 920.21 8. 745235 NU3

5 5 3 2 508 .81 0.019115 NU3

4 7 2 5 782 .40 6.352023 NU3

3 4 3 2 382.52 1.848533 NUl

5 5 1 4 399.46 1.912338 NUl*

4 7 3 5 816.72 2.323327 2NU2

7 8 0 8 2337.53 7.747248 NU3***

7 8 1 8 2337.70 7.746063 NU3***

4 7 3 5 816.72 4. 550000 NU3-

4 4 2 3 300.35 1.5673.00 NUl*

3 4 0 4 222.06 2.831638 NUl**

2 6 3 3 661 .56 3. 180000 NU3*

2 5 4 1 610.35 4.266963 2NU2*

5 7 1 6 704.22 6.391209 NU3*

3 6 2 4 2211,21 5.358633 NU3***

40
LINE HALF

FREQUENCY STRENGTH WIDTH J K cm~' cnn"i cm"i

gm cm -2 atm.

3572.23 0.3780 0. 0734 6 2 5 3572.49 0.2269 0.0699 5 4 1 3572.50 0,0120 0.0516 5 5 0

3572.53 0.0359 0.0516 5 5 1 3572.76 4.6660 0.0840 8 2 6

3573.06 0 .0403 0.0871 5 0 5

3573.08 0.6543 0.0644 7 5 2

3573.23 0.0592 0.0955 2 1 2

3573.39 0.0743 0.0850 4 4 1 3573.44 0.6844 0.0679 5 4 2

3573.63 34,7936 0.0833 3 2 2 3573.65 0.2203 0.0835 3 2 1 3573.88 0.0542 0.0907 4 1 4

3574.07 0,5616 0.0535 7 0 7

3574.11 1,6840 0.0532 7 1 7

3574.47 130,4987 0.0974 3 1 3

3574.81 0,1950 0.0797 5 3 3

3575.06 35,6751 0.0952 3 0 3

3575 .09 0,0591 0.0951 3 2 2

3575. 10 0,0394 0.0909 4 3 2

3575.80 0 . 1464 0.0546 11 2 9

3576.49 0 .0408 0.0835 3 2 1 3576.73 0.2971 0. 1006 2 0 2

3576.85 108.9735 0.0871 5 0 5 3577.21 146.6057 0.0907 4 1 4

3578.04 0,0240 0.0942 4 0 4

3578.04 4,2064 0.0762 4 2 2

3578.06 0,7885 0.0917 5 2 3

3578,73 0,0511 0.0509 12 3 10

3578.90 0,0644 0.0861 5 3 2

3579.30 0,3138 0.0785 6 1 5

3579.33 110,1731 0.0835 3 2 1 3579.60 0,0699 0.0734 6 2 5

3580.09 32,3977 0.0516 5 5 0

3580.12 97.1937 0.0516 5 5 1 3580.26 1.1817 0.0797 5 3 3

3580.43 0.0137 0.0886 7 2 5 3580.99 3.1751 0.0451 9 0 9

3581.03 0.1266 0.0679 5 4 2

3581.09 2,6402 0.0491 10 1 9

3581.29 0 ,1406 0. 1037 1 0 1 3581.32 0,2278 0.0884 5 2 3

3581.38 0.1039 0.0535 7 0 7

3581.43 0.3115 0.0532 7 1 7

3581.48 0.0488 0.0971 2 0 2

3581.63 0.0241 0.0459 8 7 2

3582.01 0.0496 0.0893 6 2 4

3582.32 9.6106 0.0458 9 1 9

3582.73 44.5822 0.0862 4 2 2

3583.28 0.2945 0. 0684 7 0 7

3583.34 29.5317 0.0951 3 2 2

3583.60 148.5278 0. 1006 2 0 2

3583.70 36.9029 0.0886 7 2 5

3584. 15 0,0421 0.0884 5 2 3

J" Kc E" L BAND

cm"!

1 d. D

"7 n O A /, '3 Q n n n r\ '+. jyuouu

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CS-/ X VJ • X A . 3AR783 NU 1

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9 Q "3 1 A -3 D Ml 1 1 IN U 1 AO j> A•-r A7 A7 7( 1X .70 . f U ^."^70000 Ml 1 ^ •«•>(• ){ A

H- A c o 1 1 A n R R Ml 1 "3 A*+ 1 A 1 ^ . A Nl 1 1 -Sr

c,J A 446 . "^n O.^'^AO^.'S NU 1 *

^ 1 X X AH- ft 1X 843.02 U " _J • \J ^ 0.981 S S9 NU3

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•3 1 ft n o o o Ml 1 -)c -}(- 7 11 Au 704 - ? 7 ALJ._77XAi^^7 . 39 1 ? 09

2 8 5.43 1 .092505 NU 1 7 9A A 7 n 9 . 6 n 4 - 390000 NU3''^'*^ AD

c,J

1X ft ft ft .A3 1.8451 X.OH-_^XOAft? NU 3 AO

9A ft ft ft AO 1 Rli'^ 1 ftO NlINU1 9 AO 5 A A AD q 7 •3 "370000 Nl 1 "3 )<

IN w 9 7 •:3 z> A ftO

A 9 "3 ft H- A . ^ O R q 1 ft A 1 1 N 1 1 1 1 N X q 9A

QO 1 n ft n ft X U O U . J o O Zl 7 1 A. 1 7 Ml 1 "3 IN U 9 AO

A 7 c; A . 7 R '^.'^RlAZi.ft MU3**

1 n 8 1 44A . 1 A 0 ft 1 8434 NU 3

C—? 1± 9 1 677.08 1X9- 500000 ^ \J \J \J \J \J NU 1 *4t-Jr R nU RO R 1 • O 1

O. A A 9 Q n 1 Ml) 1

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1 N V-/ X

ft nu ftO 7 44 - HQ 7-747 1 • / H- f ^? 4ft *-r O

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TX AO 7 - 74 A OA NU 3 •«)«•

-J 9A X 1 8 1 Q * '^4 X O X 7 • _? H 0.0Q44Qft

9 AO X U -J X • M- X 0- 1 Q7ftQ8 NU1 "1 w X1 A •3—

A A 1 . R A 4.8 ? 94^ 5 NU 1-^ 9 11 R(J 1 0 79- 07 0.47731

8

w . H- f A 9 X U NU 3

A -3J X J O .0-3 A.iOlAA9 9 1 A 7 9 9 R INM 1Un1 AD :5 A A AD q 7 O O 1 7 q A O MlIN VJM1 A

i A /9.9a n ft 5 n q R Mill IN U 1

i i X M-^ . ^ O

9 1 A "7 Q 9 A. i9D (Va Mill IN U i 7 3 4 842.38 5.918411 NUl

5 3 2 508 .81 3.442901 NUl^-K707-944 O 64 - 4 41
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm ' gm cm"

2

atm.

3584.34 19 ,6813 0.0909 4 3 2

3585.00 0,0092 0.0893 6 2 4

3585 , 14 0.0365 0.0692 6 0 6

3585.21 25.6035 0.0743 6 4 2

3585,62 0. 1458 0.0917 5 2 3

3585.67 0.1804 0.0872 5 1 4

3585,84 2 .7719 0.0792 5 2 3

3586. 56 848 .0212 0.0785 6 1 5

3586.62 174.0871 0,0861 5 3 2

3586.87 0,1818 0.0709 7 3 5

3586.97 188,9975 0.0734 6 2 5 3586.98 7.8862 0.0598 6 5 2

3586.99 113 .8876 0.0884 5 2 3

3587,32 2.6308 0.0587 6 5 1 3587,50 29.1302 0.0877 6 1 5 3587,75 113 .4523 0.0699 5 4 1 3587,80 0,2186 0.0797 5 3 3

3587,99 24,8189 0.0893 6 2 4

3588,37 0.3947 0.0818 5 2 4

3588,63 342.1935 0.0679 5 4 2

3588,70 280.8225 0.0535 7 0 7

3588.76 842 .0047 0.0532 7 1 7

3589. 53 0.9367 0.0516 10 2 9

3589.75 0.1402 0.0845 4 0 4

3589.75 1.3763 0.0620 10 2 8

3590. 13 0.1278 0.0638 4 4 0

3590.23 64.9916 0.0944 3 1 3

3590.26 0.1231 0.0937 3 1 2

3590.47 0.5364 0.0649 6 C 6

3590.62 0.7425 0.0994 2 1 2

3590,64 0.1786 0.0642 6 1 6

3590.83 0.0584 0.0553 7 6 2

3591 . 30 0.1826 0.0762 6 0 6

3591.59 0.1759 0.0527 7 6 1 3591.69 0.2267 0.0711 7 1 6

3591.76 0.0236 0.0780 6 3 3

3591.95 0.1455 0.0942 4 0 4

3592.33 1 .0936 0.0872 5 1 4

3593. 19 394,2654 0.0917 5 2 3

3593.45 3,7532 0.0862 4 1 4

3593.48 0,3588 0.0955 2 1 2

3593.79 0,6888 0.0816 5 0 5 3593.99 10 .3074 0.0803 6 2 4

3594, 04 0.8524 0. 1037 1 0 1 3594. 36 0.1374 0.0994 2 1 2

3594. 52 3.2509 0.0649 6 0 6

3594.62 1 .0318 0.0642 6 1 6

3594.72 0,0219 0.0840 5 4 2

3595.35 590,8837 0.0797 5 3 3

3595.48 1.0175 0.0704 6 5 2

3595 .94 0,3824 0.0912 5 1 4

3596. 17 66,3420 0.0840 5 4 2

3596,72 0,0664 0.0955 2 1 2 3596,82 0,0241 0.0431 8 7 1

1" F" 1 BAND

5 2 3 446 . 50 0.436045 NUl

6 3 3 661.56 4.829435 NU 1**

5 4 1 610.35 0 . 000 1 72 NU3

7 3 5 816.72 10.83 NU1 +

6 2 4 602.77 5. 358633 NU3**

6 1 5 2146.28 5 . 48 8405 NU3***

5 4 2 610.12 0.039164 NU3

7 1 6 704.22 6.391209 NU3

6 3 3 661 . 56 3.180000 NU3-

6 0 6 446 .71 0. 130226 2NU2

1 2 6 709.60 4.390000 NU3-

5 4 1 610.35 4. 266963 2 NU 2

5 3 2 508.81 3 . 44290

1

NUl

5 4 2 610.12 4. 264570 2NU2

6 2 4 602.77 4.225862 NU 1 6 4 2 757.78 3.352166 NU3

6 3 4 648 .97 3 .370000 NU3**

6 3 3 661 . 56 4. 829435 NUl

6 2 5 2161.30 4. 200000 NU3***

6 4 3 756.75 3.351648 NU3

8 0 8 744 . 09 7 . 747248 NU3

8 1 8 744 .16 7. 746063 NU3

10 2 8 1438.00 0. 834303 NU3

3 3 1 285.23 0.004153 NU 1

1

0

4 7 1 58 1 . 34 0.828214 NU3

5 4 1 2251 .86 1.810956 NU3***

3 2 2 206.30 1.297651 NUl

3 2 1 1819.34 2.538253 NU l*^*

7 0 7 2180.65 6.749914

3 0 3 136.77 1 . 741 385 NU l-"-*- 7 1 7 2181.12 •6. 746361 NU3***

8 5 3 1255.92 0.222252 NUl

5 3 3 504 . 00 0.016149 NUl

8 5 4 1255.16 0.221954 NU 1 6 4 3 756.75 0.023637 NUl

7 2 6 2318,53 17,68 NU I***

4 1 3 275,52 2 . 047924 NUl*

6 1 5 542,91 5.48 8405 NU3*

6 2 4 602,77 5.358633 NU3

4 3 1 383,85 0.017070 NU3

2 2 1 134,91 0. 833333 NU 1*

4 3 2 382 .52 0.011053 NUl

6 4 3 756.75 0.100806 NU3

2 1 2 79 .48 1 . 500000 NUl*

3 0 3 136.77 1.741385 NUl**

7 0 7 586.26 6.749914 NU3*

7 1 7 586.48 6 . 746361 NU3*

6 3 3 2282.59 12.78 NUl***

6 3 4 648 . 97 3.370000 Ml 1 O NU 3 —

7 4 3 931.22 0.253734 NU 1 5 2 3 446 . 50 4.214107 NUl*

6 3 3 661 .56 12.78 NU 1 +

2 2 1 134.91 0.833333 NUl**

8 6 2 1411.68 2. 144937 2NU2

42
FREQUENCY

LINE HALF

STRENGTH WIDTH J' cm~' cm 1 cm-1

gm cm -2 0 tm.

3596 .85 0.0723 0 . 0430 8 7 2

3597.08 0.3203 0.0 826 3 1 3597.21 0,0183 0.0870 3 1 3

3597.25 0 ."l 2 8 8 0.0975 3 0 3

3597.51 0,1577 0. 1037 1 0 1 3597.62 2 .3918 0.0818 5 2 4

3598. 11 371 .2599 0. 0994 2 1 2

3598.58 71.6598 0.0780 6 3 3

3598.87 1 .1526 0.0694 9 2 7

3598 . 94 0.3418 0.0626 6 5 1 3598.97 0.2957 0.0971 2 0 2

3599.07 0.6819 0.0920 2 2

3599.24 0. 7743 0.0638 4 4 0

3599.45 0.25 84 0.0633 4 1 3599. 46 19.1232 0.0737 7 3 4

3599.46 72.7472 0.0942 4 0 4

3599.68 0.2023 0.0872 5 1 4

3599.97 179.3981 0,0955 2 1 2

3600.22 3.1696 0.0791 7 2 5

3600 .75 2 .6347 0.0570 9 1 8

3600.98 426 . 1887 0. 1037 1 0 1 3601 . 04 265.5457 0.0814 5 3 2

3601 .87 0.6015 0 . 0649 6 0 6

3601.99 0.2001 0 .0642 6 1 6

3602 .32 1 .941

1

0.0826 3 1 3602 .33 6.6223 0 .0747 8 2 6

3602 . 55 24.8739 0.0531 8 0 8

3603.05 191 . 2005 0.0912 5 1 4

3603.86 0 . 0409 0 .0663 8 1 7

3604 .36 4. 1325 0.0920 2 2

3604.48 0,0108 0.0838 L, 4 0

3604 .65 0.2061 0.0801 8 1 8

3605 . 08 0,4425 0.0818 5 2 4

3605.27 0,2123 0.0934 4 1 3

3605 .29 8 .4594 0. 0547 8 1 8

3605 , 74 0 .4620 0.0798 9 4 5 3606 .01 0 .7798 0 .0803 4 3 2

3606 .02 0.0547 0.0971 2 0 2

3606. 34 0,0177 0 .0949 2 2 1 3607.03 546 ,7939 0 .0872 5 1 4

3607.25 4 ,5897 0. 0727 5 4 1 3607 .39 0.9355 0.0926 4 1 3

3607.86 0.1803 0.0957 2 1 1 3608.01 0.6081 0.0596 1

1

3 9

3608 ,31 0.0271 0 .0427 7 7 0

3608 . 46 0.0389 0,0636 7 0 7

3608.64 0.0393 0.0 934 4 1 3

3608 .73 0.7459 0.0937 3 1 2

3609 .21 0.0127 0,0 829 4 3 1 3609.23 1625.4689 0. 0649 6 0 6

3609 . 36 540 .9480 0 . 0642 6 1 6

3609 . 99 0.3591 0.0826 4 3 1 3610.12 9.1514 0,0870 3 1 3

3610.31 0.0604 0. 1021 2 0 2

J" Kc E" L BAND

4 cm 1

8 6 3 1411.65 2 , 144879 2NU2

5 3 2 2130 . 50 2 . 730000 NU3***

3 3 0 285.43 0.008443 NU3*

3 1 2 1772 .41 2, 185861 NUl***

2 1 2 79.48 1 . 500000 NUl**

6 2 5 552.92 4. 200000 NU3*

3 0 3 136.77 1.741385 NUl

7 2 6 709 . 60 17.68 NU1 +

9 4 6 1340.89 0.624317 NU3

7 4 4 927.77 0.250934 NUl

3 2 1 212.15 0.094498 NU3*

5 2 3 2053.98 4. 253846 NU3***

5 4 1 610.35 1.810956 NU3*

5 4 2 610.12 1 .810924 NU3*

8 2 7 885,62 3. 79 NU1 +

4 1 3 275,52 2 . 047924 NUl

6 1 5 542 ,91 5. 488405 NU3**

2 2 1 134,91 0.833333 NUl

7 4 4 927.77 0.218314 NU3

9 3 7 1216.27 0. 769552 NU3

2 1 2 79 .48 1 . 500000 NUl

6 2 5 552.92 9.87 NU1 +

7 0 7 586.26 6 , 749914 NU3**

7 1 7 586 .48 6 , 74636

1

NU3**

5 3 2 508.81 2. 730000 NU3*

8 4 5 1122.72 0,402567 NU3

8 2 7 885.62 0.462205 NU3

5 2 3 446 . 50 4.214107 NUl

8 3 6 1006 . 12 0.691047 NU3*

5 2 3 446 . 50 4. 253846 NU3*

3 1 3 142 .28 0.001674 2NU2

7 2 5 782 .40 0.024347 NUl

6 2 5 552.92 4. 200000 NU3**

4 2 2 315.79 3. 642913 NUl*

8 1 7 882 .93 0.464983 NU3

8 3 6 1006. 12 1,797448 2NU2

5 3 3 504 .00 3.208780 NU3*

3 2 1 212.15 0.094498 NU3**

3 1 2 1772.4-1 0. 300506 IMUl***

6 1 5 542 .91 5.488405 NU3

6 3 4 648 .97 0.278030 NUl

5 1 4 2000 .90 4.601931 NU3***

2 2 0 136.17 1.258755 NUl*

1

1

3 8 1813.26 1 . 122765 NU3

8 6 3 1411.65 0.074321 NUl

7 2 6 . 709.60 0. 448059 NU3*

4 2 2 315.79 3. 642913 NUl**

3 2 1 212.15 2. 538253 NU1*«

5 2 4 2024.17 2.18 NUl***

7 0 7 586 . 26 6 . 749914 NU3

7 1 7 586 .48 6 . 746361 NU3

5 3 2 508.81 2. 730000 NU3**

3 3 0 285.43 0.008443 NU3

2 1 1 1693.65 2.074578 NUl***

43
LINE HALF

FREQUENCY STRENGTH WIDTH J' J" Ka E" L BAND rm i cm ' cm-1 cm-1

gm cm -2 arm.

361 0.39 0 ,0775 5 0 5 6 0 6 2041 .76 5. 755360 NU3***

\j J, \j » \j \j 0 - 7804 0, 0975 3 0 3 3 1 2 173 .36 2. 185861 NU 1*

^61 n . 74 1 - 7796 0,0660 7 5 3 6 4 2 757.78 4. 143594 2NU2

^ O 1 u • o u n * Q 1 QQ 0 , 0 764 5 1 5 6 1X 6 2042 . 77 5 . 744669 NU3***

-3 U J, X • U ( V • VJ _^ J _/ 0. 0957 2 1 1 2 2 0 136 .17 1.258755 NU I**

^ w X X • X O 0-0198 0. 0949 2 2 1 3 2 173 .36 0.300506 W» -/WW^WW NU 1**

^ U X X • ^ X 0.0791 V • V <^ 7 X 0 . 0994 1 0 1 2 2 0 1743 .47 0\J .038246 9 W ^ t- ~ W NU3***

3611.87 3.6986 0.0628 7 5 2 6 4 3 756.75 4.131192 2NU2

36 1 1 . 99 0. 1380 0 .0937 3 1 2 3 2 1 212.15 2.538253 NUl**

3612.00 0.7645 0.0920 4 2 2 5 2 3 446 . 50 4. 253846 NU3**

3612.02 106.1695 0.0934 4 1 3 4 2 2 315 .79 3.642913 NUl

^ 'u' X • ^ V 1 195 .9086 0.0818 5 2 4 6 2 5 552.92 4.200000 NU3-

3613.07 147.8754 0.0971 2 0 2 3 2 1 212.15 0.094498 NU3

3613.42 5.6696 0.0926 A- 1 3 5 1 4 399 ,46 4.601931 NU3*

3613.59 0.1 442 0.0803 4 3 2 5 3 3 504,00 3 . 208780 NU3**

3613-89 0.01 77 0.0557 7 4 4 6 6 1 1 045 , 07 0. 000730 NU3

3614-78 90. 1255 0.0957 2 1 1 2 2 0 136,17 1 .258755 NUl

'^81 4 • 44 387.1 051 0.0638 4 0 5 4 1 610,35 1.810956 NU3

361 4.64 179 . 7037 0.0633 4 4 1 5 4 2 610,12 1. 810924 NU3

3614.69 1 .8667 0 •0115 5 0 5 6 0 6 446 .71 5. 755360 NU3*

3614 . 84 5.5753 0 .0764 5 1 5 6 1 6 447 . 24 5 • 744669 NU3*

3615.25 372 .9500 0.0937 3 1 2 3 2 1 212.15 2.538253 NUl

3615.35 53.6079 0.0949 2 2 1 3 1 2 173 . 36 0. 300506 NUl

3615.58 0.1841 0.0875 4 2 3 5 2 4 2024,17 2 . 950000 NU3***

3615.60 0.1733 0. 1044 1 1 1 2 0 2 70 .08 0.755253 NUl*

3 615.64 3 8-4970 0.0829 4 3 1 5 2 4 416 ,22 2.18 NUH3615.79 9.0578 0.0606 9 2 8 9 2 7 1201.95 0.8 13942 NU3

-SAT A . on v> . U U X ^ 0 .0846 6 4 3 5 4 399,46 0.071290 2NU2

3617.66 970.5790 0.0826 4 3 1 5 3 2 508 ,81 2 . 730000 NU3-

3617.99 390 .2244 0.0975 3 0 3 3 1 2 173 ,36 2.185861 NUl

-J U X O . X D 0 .0663 8 1 7 8 3 6 1006 , 12 0. 691047 NU3

0 - 060

1

V •WWW X 0.0497 6 6 0 7 5 3 1059,65 0 .084869 NUl

3618.36 0.0790 W # W t 7 W 0 .0743 7 1 6 7 3 5 8 16 , 72 0. 567704 NU3*

3618 .85 1.1157 X « X X ^ ' 0.0875 4 2 3 5 2 4 416,22 2. 950000 NU3*

3619-4? 4-7191 ~ • t X 7 X 0. 0884 3 3 1 4 2 2 315 , 79 0.161593 NUl

3619 . 64 7^WWW 066 .73 9 ^ J 76 0.0920 4 2 2 5 2 3 446 ,50 4. 253846 NU3

3619.95 141 X ~ X .6631 • W W ^ X 0 .0996 0 0 0 1 1 1 37,13 1 . 000000 NUl

3620.88 1 . 0489 0.0926 4 1 3 5 4 399 ,46 4. 60 193

1

NU3**

3621.17 389.8899 0, 0803 4 3 2 5 3 3 504, 00 3. 208780 NU3

3622 . 07 0.3454 0.0775 5 0 5 6 0 6 446.71 5.755360 NU3**

36?? - ?5 1X -# 03W 1X 4*T 0 • 0764 5 1 5 6 1 6 447.24 5. Iht^beS NU3**

J D ^ 3 • 1 7 TO A ft A A nW .• 0636 w w w 7 0 7 7 9 6 709.60 0.448059 NU3

J \J C. Sj • ^ J? 0.1 044 X 1 1 2 0w 2 70 . 08 0.755253 NUl

0W .# J Aw AW _J 0.1021 2 0 2 2 X1 1 95.17 2 . 074578 NU 1*

3624.02 3.7777 0 .0646 5 5 1 6 4 2 757.78 1 . 02 NU1 + 3624.24 0,1295 0 .0784 3 3 0 4 3 1 2005.92 1. 758969 NU3***

3624 . 54 0.0560 0.0633 9 3 6 10 2 9 1293 .66 0.084934 NUl

3625.05 9.871

7

7 W ( X fc. 0. 0590 5 5 0 6 4 3 756.75 1 . 02 NU1 + 3675.17 0-391

1

W * J 7 X X 0,0774 3 3 1 4 3 2 2004.81 1.758385 NU3***

3675 - 48 0-01 w • W X 50^ w 0.0773 6 1 6 6 1 5 2 146 , 28 0.450603 NU3***

3626.24 153.1589 0.0787 4 4 1 5 3 2 508 .81 4.58 NU1 + 3626.35 0.2064 0.0875 4 2 3 5 2 4 416.22 2.950000 NU3**

3626.72 0.0180 0.0689 8 2 7 8 2 6 982.91 0.807542 NU3*

3626.80 0,3139 0.0914 3 2 1 4 2 2 1922.92 3.033776 NU3***

44
LINE HALF

J Kq FREQUENCY STRENGTH WIDTH K

rm cm ~^ gm cm 0 tm

3627.12 0.0678 0. 1021 2 0 2

3628. 34 2834.7985 0.0926 4 1 3

3628.70 61.3129 0.0654 7 1 7

3629.45 933.3359 0.0775 5 0 5 3629.66 2787.6639 0.0764 5 1 5 3629.91 1 .4124 0.0887 4 0 4

3630.71 183. 1462 0. 1021 2 0 2

3630.80 1 .3310 0.0708 4 4 0

3630.80 0.4647 0.0957 3 1 2

3631.00 1.0367 0. 1075 1 0 1 3631.21 0.7850 0.0784 3 3 0

3631 .79 1 .9028 0.0914 3 2 1 3632.15 0.0343 0.0914 3 2 1 3632.24 14.4900 0.0743 7 1 6

3632.35 2.3704 0.0774 3 3 1 3632.49 0.1218 0.0871 4 1 3

3632.91 0.0541 0.0857 5 1 4

3633.86 557.8829 0.0875 4 2 3

3633.88 1 .5055 0.0706 8 5 4

3634.42 8.5598 0.0887 4 0 4

3634.54 0.1918 0.1075 1 0 1 3635.00 12.4966 0.0829 3 3 0

3635.10 0.0262 0.0813 6 1 5

3635.22 0.0450 0.0747 6 0 6

3635.74 2.8170 0.0872 4 1 4

3636.18 0.0457 0.0633 12 4 9

3636.22 2.8166 0.0957 3 1 2

3636.29 1.0035 0.0903 3 2 2

3636.34 0.0326 0.0994 1 0 1 3636.47 0.0137 0.0500 10 1 10

3636.47 0. 1789 0.0394 12 3 10

3637.45 0.0909 0.0773 6 1 6

3637.69 0.7973 0.0671 10 3 8

3638.09 518.3663 0.1075 1 0 1 3638.36 0.2655 0.0614 8 3 6

3638.84 0.1452 0.0784 3 3 0

3638.88 0.0226 0.0871 4 1 3

3639.45 0.3521 0.0914 3 2 1 3639.93 17.1625 0.0914 3 2 1 3639.94 26.7903 0.0872 4 2 2

3639.95 0 .4386 0. 0774 3 3 1 3641.24 6 .0815 0.0903 3 2 2

3641.61 8.4447 0.0860 3 1 2

3641.81 70.8127 0.0813 6 1 5 3641.84 1.5835 0.0887 4 0 4

3642.57 121.6832 0.0747 6 0 6

3642.99 9 .0052 0.0689 8 2 7

3643.20 0.5212 0.0872 4 1 4

3643.33 88.2494 0.0994 1 0 1 3643.55 0.1293 0.0788 7 4 4

3643.73 0.0397 0.0786 10 4 6

3643.77 0.5210 0.0957 3 1 2

3644. 12 0 .0610 0.0812 5 4 1 3644.41 0.0111 0.0649 6 5 2

J" E" L BAND

cm"!

2 1 1 95.17 2 . 074578 NU

5 1 4 399.46 4.601931 NU3

7 1 6 704.22 0.456726 NU3

6 0 6 446.71 5 .755360 NU3

6 1 6 447.24 5. 744669 NU3

5 0 5 1920.76 4.769122 NU3***

2 1 1 95.17 2.074578 NUl

5 3 3 504 .00 0. 116422 NUl

A- 1 3 1875 .49 3. 667441 NU3***

1 0 42.37 1 . 500000 NU 1*

4 3 1 383.85 1 .758969 NU3*

4 2 2 315.79 3. 033776 NU3*

4 1 4 224.83 0. 123609 NUl*

7 3 5 816.72 0 . 567704 NU3

4 3 2 382 .52 1 . 758385 NU3*

4 3 2 382 .52 0.090390 NU3*

5 3 3 504.00 0.221254 NU3*

5 2 4 416.22 2. 950000 NU3-

7 4 3 931 .22 4. 002077 2NU2

5 0 5 325.35 4. 769122 NU3*

1 1 0 42 .37 1 . 500000 NU 1**

4 2 3 300 .35 0. 131472 NUl

6 3 4 648 .97 0.398711 NU3-i^-*

6 2 5 552.92 0.423826 NU3**

5 1 5 326.64 4. 737042 NU3*

12 4 8 2205 .65 1 . 508618 NU3

4 1 3 275.52 3. 667441 NU3*

4 2 3 1907 . 99 2 . 984448 NU3***-

2 2 0 136. 17 0.038246 NU3**

9 3 7 1216.27 0. 003958 NU3

13 3 11 2248 .16 11 . 866070 NU3

6 1 5 542 .91 0. 450603 NU3*

10 3 7 1538.23 1.142576 NU3

1 1 0 42 .37 1 . 500000 NU 1 7 0 7 586.26 0.125531 2NU2

4 3 1 383 .85 1.758969 NU3**

4 3 2 382 .52 0.090390 NU3**

4 2 2 315.79 3 .033776 NU3**

4 1 4 224.83 0.123609 NUl

5 1 5 326.64 0.963 NU1 +

4 3 2 382.52 1.758385 NU3**

4 2 3 300 .35 2 .984448 NU3*

3 3 1 285.23 0.023148 NU3

6 3 4 648 .97 0.398711 NU3

5 0 5 325.35 4. 769122 NU3**

6 2 5 552.92 0.423826 NU3

8 2 6 982.91 0.807542 NU3

5 1 5 326.64 4. 737042 NU3**

2 2 0 136.17 0.038246 NU3

6 1 5 542 .91 0. 147419 2NU2

9 3 7 1216.27 1 .314980 2NU2

4 1 3 275.52 3 . 667441 NU3**

4 1 4 224.83 0.004729 2NU2

6 2 5 552.92 0.004423 2NU2

45
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq K cm-1 cnn~i rm ~ 1 gm cm ~ 2 atm.

364-^.66 0.0299 0.0424 8 6 3

3644.71 0.0100 0.0424 8 6 2

3645. 10 0.1019 0.0401 7 7 0

3645.28 60.8873 0.0871 4 1 3

3645,41 0.1445 0.0846 5 0 5 3645.62 0.0302 0.0628 8 4 4

3645.94 27.0677 0.0857 5 1 4

3646.47 392.4581 0.0784 3 3 0

3647.12 951 .3782 0.0914 3 2 1 3647.55 1185.1957 0.0774 3 3 1 3647.69 7.1283 0.0941 2 2 0

3648.56 51.0375 0.0812 5 2 3

3648.79 1.1250 0.0903 3 2 2

3649.27 4279.9025 0.0887 4 0 4

3650.66 1408 .4906 0.0872 4 1 4

3651.32 1408 ,3050 0.0957 3 1 2

3651.56 1.8287 0.0948 3 1 3

3652.39 1 .0352 0.0590 6 4 3

3652.67 0.0941 0.0863 5 1 5 3652.93 45.4636 0.0773 6 1 6

3653.64 0.0147 0.0960 3 1 3

3653.66 0.1541 0.0782 7 2 6

3653.87 3.8369 0.0960 3 0 3

3654.24 0.1779 0.0750 9 5 5 3654.32 0.8804 0.0907 2 2 0

3655.15 0.1180 0.0650 9 2 7

3655.27 0.1328 0.0562 9 1 9

3655.41 0.0259 0.0577 9 4 6

3655.71 1 1 .0833 0.0948 3 1 3

3655.77 1 .6872 0.0986 2 1 1 3656.35 3040 .7787 0.0903 3 2 2

3658.38 0.0468 0.0722 9 5 4

3658.39 0.0368 0.0948 4 1 4

3658.53 0.3008 0.0915 2 2 1 3658.54 0.0494 0.0977 2 0 2

3659.66 5.3353 0.0907 2 2 0

3659.83 0.3467 0.0629 6 4 2

3659.86 0.0272 0.0825 4 2 3

3659.87 1 .0473 0.0763 8 4 4

3659.90 0.6137 0.0916 4 0 4

3659.94 72.2409 0.0846 5 0 5 3660.36 7.3739 0.0960 3 1 3

3660.71 10.2254 0.0986 2 1 1 3661.07 0. 1896 0.1111 1 1 0

3661.33 0.7099 0.0960 3 0 3

3661 .67 2.6981 0.0929 5 1 5

3661.82 0.0285 0.0782 7 2 6

3661 .84 0.5702 0.0863 5 1 5

3662.22 1 .4535 0.0690 5 3 3

3663.07 0.2732 0.0747 6 2 4

3663.21 2 .0504 0.0948 3 1 3

3664.26 1.8233 0.0915 2 2 1 3664.28 0.5369 0.0654 9 5 4

3664.42 0.6240 0.0688 11 4 8

J" Kc E" L BAND

cm-1

7 7 0 1394.86 0.074321 NUl

7 7 1 1394.86 0.074323 NUl

7 6 1 1216.20 1. 119797 2NU2

4 3 2 382.52 0.090390 NU3

5 2 4 416.22 0.379277 NU3*

7 6 1 1216.20 0.002886 NU3

5 3 3 504.00 0.221254 NU3

4 3 1 383.85 1.758969 NU3

4 2 2 315.79 3.033776 NU3

4 3 2 382.52 1.758385 NU3

3 1 3 142.28 0. 101693 NUl

6 1 6 447, 24 1.115 NU1 +

4 2 3 300.35 2.984448 NU3**

5 0 5 325.35 4.769122 NU3

5 1 5 326.64 4.737042 NU3

4 1 3 275.52 3.667441 NU3

4 1 4 1821.61 3.713893 NU3***

5 5 0 742.10 0.098702 NUl

5 1 4 2000.90 0.456689 NU3***

6 1 5 542 .91 0.450603 NU3

2 2 0 136.17 0. 101693 NUl*

7 2 5 782.40 0.838975 NU3*

4 0 4 222.06 3.805784 NU3*

8 4 4 1131 .76 3.840219 2NU2

3 2 1 1819.34 1.676022 NU3***

8 1 8 744, 16 0.122288 2NU2

8 3 6 1006. 12 0,004442 NU3

8 6 3 1411.65 0,006585 NU3

4 1 4 224.83 3,713893 NU3--

3 1 2 1772.41 2,645088 NU3***

4 2 3 300.35 2.984448 NU3

10 3 7 1538.23 0.066606 NU3

3 2 1 212.15 0. 123509 NUl*

3 2 2 1813.81 1.666667 NU3***

2 2 1 1742.28 0,063744 NU3***

3 2 1 212.15 1,676022 NU3*

5 5 1 742 . 10 0.098971 NUl

3 3 0 285.43 0, 131472 NUl*

9 2 7 1201.95 0,092972 NU3

4 2 3 300,35 0,299684 NU3*

5 2 4 416,22 0,379277 NU3

2 2 0 136,17 0, 101693 NUl

3 1 2 173,36 2,645088 NU3*

1 0 1 1618,55 1.500000 NUl***

4 0 4 222.06 3.805784 NU3**

4 2 2 315.79 0.091324 NUl

7 2 5 782 .40 0.838975 NU3**

5 1 4 399.46 0.456689 NU3*

4 4 0 488. 13 0.116422 NUl

7 1 7 585 .48 0.035782 NUl

4 1 4 224.83 3.713893 NU3**

3 2 2 206.30 1 .666667 NU3*

8 4 5 1122 .72 3.682999 2NU2

11 4 7 1899.06 1.701473 NU3

46
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm-1

nm rrri ~ 2 cm 1 u 1 rn. 3664.61 0.0723 0.0669 10 4 6

3664.67 0.2090 0.0652 7 3 5

3665.00 4.5829 0.0431 6 6 1 3665.25 1.7589 0.0431 6 6 0

3665.41 18.4141 0.0948 4 1 4

3665.62 0.0298 0.0447 9 6 3

3665.86 4.4771 0.0761 5 3 2

3665.90 13.5789 0.0825 4 2 3

3665.95 1 .0990 0.0680 6 3 3

3666.01 9.2943 0.0740 9 3 7

3666.92 0.0954 0.0798 9 2 8

3667.01 0.0798 0. 1044 2 1 1 3667.02 1.1491 0.1111 1 1 0

3667.08 0.1136 0.0916 4 0 4

3667.31 0.9870 0.0907 2 2 0

3667.32 0.0219 0.0951 3 1 2

3668.31 1.8917 0.0986 2 1 1 3668.79 1918.4159 0. 0960 3 0 3

3668.93 2.2135 0.1010 2 0 2

3669.64 0.1055 0.0863 5 1 5

3669.98 77.0437 0.0782 7 2 6

3670.37 0.1991 0.0948 3 0 3

3670.72 5541.6353 0.0948 3 1 3

3671.35 0.0181 0.0345 8 8 0

3671.50 0.1260 0. 0620 8 1 8

3671.85 0.3373 0.0915 2 2 1 3671 .92 0.6619 0.0984 2 1 2

3672. 17 0.0104 0.0385 9 8 1 3672.74 0.4835 0. 1044 2 1 1 3673. 19 0.0732 0.0542 8 5 3

3673.23 0,2192 0.0516 8 5 4

3673.40 13.4152 0.1010 2 0 2

3674.27 306.8374 0.0916 4 0 4

3674.73 574.5293 0.1111 1 1 0

3674.97 2667.6552 0.0907 2 2 0

3675.92 5112.6901 0.0986 2 1 1 3676.55 0 .0894 0. 1044 2 1 1 3677.37 0.6079 0.0729 5 2 4

3677.44 285.1285 0.0863 5 1 5 3677.71 0.1577 0.0994 3 1 2

3678.36 0.0107 0.0749 9 4 6

3678.46 0.0570 0.0605 9 0 9

3679.44 91 1 .6467 0.0915 2 2 1 3680.24 0.7428 0.0784 7 4 3

3680.37 241 .7413 0. 1044 2 1 1 3680.92 2 .4818 0.1010 2 2 3681.00 5.5316 0.0826 5 2 4

3681.02 0.06 5 0 0.0757 7 4 4

3681 .35 5.5923 0.0864 4 2 2

3681.38 0.0652 0. 0649 8 3 6

3681.52 0.1849 0.0385 10 8 3

3681.52 0.5547 0.0385 10 8 2 3681.58 0.1811 0. 1032 2 0 2

3681.74 0.4747 0.1037 1 1 0

J" E" L BAND

cm-1

1 1 2 9 1690.70 0.075083 NU3

6 5 2 888 .60 0.003875 NU3

5 5 0 742. 10 4. 59 2iMU2-

5 5 1 742.10 5.399693 2NU2

3 2 1 212.15 0. 123609 NUl

8 7 2 1590.74 0. 197898 NUl

4 4 1 488 . 10 0. 119405 NUl

3 3 0 285.43 0. 131472 NUl

5 5 0 742 .10 0.009800 NU3 +

9 3 6 1282.92 1.235624 NU3

8 3 5 1050.15 0. 126905 NUl

2 0 2 1664.97 2.074578 NUl***

1 0 1 23 .79 1 . 500000 NUl*

4 2 3 300.35 0.299684 NU3**

3 2 1 212.15 1.676022 NU3*^«-

2 2 1 1742 . 28 0.300506 NUl***

3 1 2 173.36 2.645088 NU3**

4 0 4 222 .06 3.805784 NU3

3 0 3 1731 .89 2 .880004 NU3***

5 1 4 399.46 0.456689 NU3**

7 2 5 782 .40 0.838975 NU3

3 2 2 206.30 0. 181744 NU3*

4 1 4 224.83 3.713893 NU3

8 8 1 1789.10 15.079045 NU3*

7 3 5 816.72 0.004883 NU3

3 2 2 206.30 1 . 666667 NU3**

3 1 3 1739.51 2.653490 NU3***

9 7 2 1810.63 2. 165395 2NU2

2 0 2 70 .08 2.074578 NUl*

7 6 2 1216.20 0.222252 NUl

7 6 1 1216.20 0.221954 NUl

3 0 3 136.77 2 .880004 NU3*

4 2 3 300.35 0.299684 NU3

1 0 1 23.79 1. 500000 NUl

3 2 1 212.15 1.676022 NU3

3 1 2 173.36 2. 645088 NU3

2 0 2 70 .08 2.074578 NUl**

4 4 1 488. 10 0.001517 NU3

5 1 4 399.46 0.456689 NU3

3 0 3 1731.89 2. 185861 NUl***

10 1 9 1293 . 04 0.047764 NUl

8 2 6 982.91 0.005067 NU3

3 2 2 206.30 1 .666667 NU3

8 2 6 982.91 0.065935 NU3

2 0 2 70.08 2.074578 NUl

3 0 3 135.77 2. 880004 NU3**

4 3 1 383.85 0.261722 NUl

6 1 7 882.93 0.037317 NUl

3 3 1 285.23 0. 161593 NUl

7 5 3 1059.65 0.006488 NU3

10 8 2 2254.34 12 . 044007 NU3

10 8 3 2254.34 12 . 044007 NU3

1 1 1 37.13 0.755253 NUl*

2 1 1 1693.65 1.50C00C NU3***

47
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm~i cm~i V^l 1 1 n m ~ 2 UNI k^l 1 1 otm.

3681.92 0.2548 0.0679 7 2 5 3681.95 0.0422 0. 0639 12 5 8

3682.11 0.1526 0. 0949 3 2 1 3682.36 0.0438 0.0951 4 2 2

3682.48 0.0120 0.0663 10 6 4

3682. 55 5.6820 0.0713 6 3 4

3683.01 0.2654 0.0951 4 2 2

3683. 12 0.9247 0.0949 3 2 1 3683. 16 0.9560 0.0994 3 1 2

3683.28 0.0554 0.0977 2 0 2

3683.56 1.2365 0.0819 8 2 7

3683.72 0.7421 0.0984 2 1 2

3683.82 1.2905 0.0688 7 4 3

3683.87 0.0212 0.0831 6 2 5 3683.95 0.9122 0.0682 7 1 7

3683.96 0.0124 0.0394 8 7 2 3683.96 0.0372 0.0394 8 7 1 3684.29 0.8244 0.0362 9 8 1 3684.29 2.4731 0.0362 9 8 2

3684.55 99 . 5498 0.0948 3 0 3

3685. 16 0.0335 0. 1032 2 0 2

3685.28 0.0819 0.0947 5 2 3

3685.52 0.2891 0. 1003 1 I 1 3685.72 0,0336 0.0847 6 2 5

3686.00 0.0380 0.0367 7 7 0

3686.00 0.1139 0.0367 7 7 1 3686.02 0.1327 0.0951 3 1 2

3686.08 0.0305 0.0408 6 6 1 3686.08 0.0917 0.0408 6 6 0

3686. 18 0.3856 0.0934 4 1 4

3686.36 0.0184 0.0460 10 6 5

3686.42 0.2262 0.0979 2 2 0

3686.45 0.3438 0.0722 6 2 5

3686.49 2.8776 0.1037 1 1 0

3686.64 0.0258 0.0544 10 2 9

3686.65 0,0373 0.0979 2 2 0

3686.65 9.0416 0.0345 8 8 0

3686.65 3,0139 0.0345 8 8 1 3686.89 0.1769 0.0994 3 1 2

3687.03 0.0491 0.0951 4 2 2

3687. 26 0.1711 0.0949 3 2 1 3687.48 0.0329 0.0695 8 5 4

3688.45 6707.5601 0. lOlO 2 0 2

3688.75 90.5474 0.1032 2 0 2

3689.25 0,0246 0.0951 3 1 2

3689.36 0,0196 0.0774 6 4 2

3689.42 0,0535 0. 1003 1 1 1 3689.87 0,8302 0.0483 7 6 2

3689.90 2 .4904 0.0480 7 6 1 3689.91 0.8102 0. 1059 1 0 1 3690.27 0.3028 0.0756 6 4 3

3690.31 149.9058 0.0977 2 0 2

3690.57 10.6222 0.0831 6 2 5

3690.63 478 .0043 0. 0994 3 1 2

ill J Kq Kc

i-ii E L BAND

8 1 8 744. 16 0.024347 NUl

1 2 5 7 2300.80 2.746007 NU3

3 1 2 1772.41 2.538253 NUl***

4 1 3 1875 .49 3 . 6429 13 NUl***

1

1

4 7 1899.06 0.032530 NU3

5 4 1 610.35 0.278030 NUl

4 1 3 275 .52 3. 642913 NUl*

3 1 2 173.36 2.538253 NUl*

3 0 3 136.77 2. 185861 NUl*

2 2 1 134.91 0.063744 NU3**

7 3 4 842 .38 0. 192937 NUl

3 1 3 142.28 2. 653490 NU3**

6 5 2 888 .60 0.253734 NUl

5 3 2 508.81 0. 312103 NUl*

6 3 4 648 ,97 0.005077 NU3

8 7 1 1590.74 11.468981 NU3*

8 7 2 1590.74 11.468981 NU3*

9 8 2 2009.87 13.413519 NU3

9 8 1 2009.87 13.413519 NU3

3 2 2 206.30 0. 181744 NU3

1 1 1 37.13 0.755253 NUl**

5 1 4 2000.90 4.214107 NUl***

0 0 0 0 .00 1 .000000 NUl*'

6 2 4 602.77 1. 202000 NU3**

7 7 1 1394.86 13.092131 NU3*

7 7 0 1394.86 13.092131 NU3*

2 2 1 134.91 0.300506 NUl*

6 6 0 2734.00 11. 108831 NU3***

6 6 1 2734. 00 11 . 108831 NU3***

4 1 3 275 .52 0.495229 NU3*

9 7 2 1810.63 0.354752 NUl

2 1 1, 95.17 1.258755 NU 1*

5 4 2 610.12 0.004724 NU3

2 1 1 95.17 1.500000 NU3*

9 4 6 1340. 89 0.013637 NU3

2 1 1 1693.65 1.258755 NUl***

8 8 1 1789. 10 15 .079045 NU3

8 8 0 1789. 10 15 . 079045 NU3

3 0 3 136.77 2. 185861 NUl**

4 1 3 275 . 52 3. 642913 NUl**

3 1 2 173.36 2. 538253 NUl**

9 2 7 1201 .95 0. 030877 NUl

3 0 3 136.77 2.880004 NU3

1 1 1 37.13 0. 755253 NUl

2 2 1 134.91 0.300506 NUl**

5 1 5 326.64 0.007497 2NU2

0 0 0 0 .00 1 . 000000 NUl**

6 5 1 888.63 5 . 265494 2NU2

6 5 2 888.60 5. 265222 2NU2

2 0 2 1664.97 1.961754 NU3***

7 1 6 704.22 0,023637 NUl

2 2 1 134.91 0,063744 NU3

5 3 2 508 .81 0, 312103 NUl

3 0 3 136.77 2, 185861 NUl

48
LINE HALF

FREQUENCY STRENGTH WIDTH J'

gm cm~2

cm 1 U ini.

3690.88 1 1 .5899 0 . 0 798 8 3 6

3691.06 132 .6981 0.0951 4 2 2

3691.28 2005 .8259 0 . 0984 2 1 2

3691 .40 462.3283 0 . 0949 3 2 1 3691 .84 0.5808 0.0757 6 1 6

3692.07 0.5537 0.0837 4 1 4

3692.21 0.0378 0.0531 9 3 7

3692.49 0.0918 0 . 0947 5 2 3

3692.49 66.3550 0.0951 3 1 2

3692.58 0,1683 0. 0994 3 0 3

3692.69 1 .5451 0.0989 1 1 1 3692.93 0.0196 0 .0509 9 6 4

3693.31 144.5340 0 , 1 003 1 1 1 3693.77 0.1230 0.0619 9 3 7

3693.80 90.9143 0 .0847 6 2 5

3694. 12 0.2496 0.0735 8 5 3

3694. 12 0.5323 0,1037 1 1 0

3694.24 4.9105 0,1059 1 0 1 3694.29 0.4194 0,0439 10 7 4

3694.29 1.2583 0 , 0439 10 7 3

3694.38 2 .3349 0,0809 5 1 5

3694.41 0.1029 0,0927 7 3 4

3694. 52 0.2451 0,0827 7 3 5

3694.80 113.0859 0 ,0979 2 2 0

3695.02 0.2268 0,0594 9 2 8

3695.24 0.0170 0,0927 7 3 4

3695.39 0.0221 0 , 0487 8 6 3

3695.59 0.0664 0,0487 8 6 2

3695.63 0.9062 C . 0691 7 2 6

3695.69 0.1889 0.0887 5 2 4

3696.34 248.1606 0. 0947 5 2 3

3696. 53 0.9272 0 .0640 8 4 5

3696.61 0.0487 0.0 529 9 5 5

3696.92 1.8803 0 . 0421 9 7 2

3696.92 5.6408 0.0421 9 7 3

3696.96 0.1915 0. 1054 2 1 2

3697.01 9.3640 0.0989 1 1 1 3697.10 0.0143 0 . 0947 4 1 3

3697. 12 0.1467 0.0586 9 5 4

3697. 16 0,0499 0.0588 7 5 3

3697.44 0.0166 0,0 588 7 5 2

3697.55 0,0676 0.0451 7 6 1 3697.55 0,2029 0.0451 7 6 2

3698.06 2,0800 0.0809 6 3 3

3698. 13 0,1759 0 . 0642 8 2 7

3698.24 0,0886 0.0721 7 3 4

3698.33 0.3215 0.0909 5 3 2

3698.46 0.1957 0. 0974 4 1 3

3698. 54 0.0190 0.0927 7 3 4

3698.79 0.0136 0.0898 8 3 5

3698.83 0.0460 0 . 0 546 6 2

3698.89 0.1379 0 . 0 546 5 1 3699.26 6.1927 0.0394 8 7 2

3699.26 18.5782 0.0394 8 7 1

J" Ka Kc E" L BAND

cm-1

8 3 5 1050.15 1.436963 NU3

4 1 3 275. 52 3. 642913 NUl

3 1 3 142 .28 2. 653490 NU3

3 1 2 173.36 2.538253 NUl

5 3 3 504.00 0.004689 NU3

3 3 1 285.23 0.001497 NU3

8 0 8 744. 09 0. 116343 2NU2

5 1 4 399.46 4.214107 NUl^-^^

2 2 1 134.91 0.300506 NUl

2 1 2 1677 .08 1.741385 NUl***

2 1 2 1677.08 1 . 500000 NU3***

9 6 3 1631 .41 7,297946 NU3*

0 0 0 0.00 1,000000 NUl

8 5 4 1255 . 16 0.014160 NU3

6 2 4 602 .77 1.202000 NU3 +

9 3 6 1282 .92 0.032937 NU3

2 1 1 95.17 1 . 500000 NU3**

2 0 2 70.08 1.961754 NU3*

10 7 3 2054.40 9.075340 NU3

10 7 4 2054.40 9.075340 NU3

4 3 2 382.52 0.003420 NU3

7 2 5 782.40 5.918411 NUl*

7 3 4 842 .38 1.781698 NU3*

2 1 1 95.17 1.258755 NUl

8 4 5 1122.72 0.013441 NU3

7 2 5 2392 . 58 5.918411 NUl***

8 6 2 1411.68 8.307617 NU3*

8 6 3 1411.65 8.307617 NU3*

6 4 3 756.75 0.008618 NU3

5 2 3 2053.98 1. 147395 NU3***

5 1 4 399.46 4.214107 NUl

7 5 2 1059.85 0.427306 NUl

8 6 2 1411 .68 0.391127 NUl

9 7 3 1810.63 10. 162962 NU3

9 7 2 1810.63 10. 162962 NU3

1 0 1 1618.55 1. 500000 NUl***

2 1 2 79.48 1.500000 NU3*

3 2 2 1813.81 0.835095 NUl***

8 6 3 1411.65 0.393126 NUl

7 5 2 2724.19 6,486001 NU3***

7 5 3 2724.05 6,486001 NU3***

7 6 2 1216.20 9,538170 NU3*

7 6 1 1216.20 9,538170 NU3*

5 4 2 610. 12 0,303663 NUl

7 4 4 927.77 0.011793 NU3

6 5 1, 888.63 0.004886 NU3

5 2 3 446. 50 3.442901 NUl*

4 0 4 222 .06 2.047924 NUl*

7 2 5 782.40 5.918411 NUl**

8 2 6 982.91 6.368783 NUl*

6 5 1 2552.87 7.626602 NU3***

6 5 2 2552.85 7.626602 NU3***

8 7 1 1590.74 11.468981 NU3

8 7 2 1590.74 11.468981 NU3

49
LINE HALF

J' Kq FREQUENCY STRENGTH WIDTH

cm~i cm ' gm cm-2 otm.

3699. 38 0.0812 0.0920 6 2

3699. A7 0.1851 0.0408 6 6 1 3699.47 0.5555 0.0408 6 6 0

3699.49 0.7748 0.0646 11 5 7

3700. 10 1.4118 0.0740 7 3 5

3700. 15 0.1145 0 . 0486 5 5 0

3700. 15 0.3436 0.0486 5 5 1 3700.65 0.0274 0.0633 9 5 5

3700.76 0.3862 0.0971 3 1 3

3700.92 0.4878 0.0952 2 2 1 3700.93 0.0190 0.0581 10 3 8

3701.30 18.9961 0.0367 7 7 0

3701 . 30 56.9884 0.0367 7 7 1 3701.58 0.5239 0.0532 11 6 6

3701.75 1438.7777 0. 1037 1 1 0

3701.78 192.7970 0.0934 4 1 4

3702.68 51 .4549 0.0927 7 3 4

3702.89 0.0595 0.0909 5 3 2

3703.01 0.0150 0.0920 6 2 4

3703.01 1.1452 0.0887 5 2 4

3703.04 0.0041 0.0487 8 6 3

3703.23 1 .1604 0. 1054 2 1 2

3703.24 0.0123 0.0487 8 6 2

3703. 57 0.0727 0.0532 10 5 6

3703 .64 0.2508 0.0865 5 3 3

3703.77 0.0341 0.0751 8 4 5 3703.83 8.3690 0.0801 6 3 3

3703.94 0.9218 0. 0754 7 3 4

3704. 14 0.0102 0.0887 9 4 5 3704.39 0.0132 0.0770 11 3 9

3704.56 1 .0200 0.0994 3 0 3

3704.60 1 .7324 0.0989 1 1 1 3704.72 0.0323 0.0614 8 5 4

3705.06 0 .1749 0.0532 11 6 5

3705.07 0.0902 0.0952 2 2 1 3705.20 0.2286 0.0536 12 6 6

3705.20 0.0126 0.0451 7 6 1 3705.20 0.0376 0.0451 7 6 2

3705.24 0.7952 0.0520 10 6 5

3705.27 5.5085 0.0845 5 3 2

3705.41 17.1589 0.0925 6 3 3

3705.49 0.9451 0 .0880 4 3 2

3705.75 97.8469 0.0974 4 1 3

3705.77 0.6215 0.0680 8 0 8

3706.37 6.7804 0.0898 8 3 5

3706.54 2 .3864 0.0520 10 6 4

3706.64 0.4168 0. 0845 6 3 4

3706.64 40.5980 0.0920 6 2 4

3706.65 0.0973 0.0614 8 5 3

3706.68 2.3406 0.0971 3 1 3

3706.78 12.9838 0.0746 9 4 6

3706.88 0.1300 0 .0884 4 3 1 3707. 12 0.0342 0.0408 6 6 1 3707.12 0.1028 0.0408 6 6 0

J" Q E" L BAND

AO11 H- A . J X. U P ? S ft A 7 IN U 1 6 0 1045.07 1 1 « 1 0 8 83 1 NU3*

6 6 1 1045 . 07 11.108831 NU3*

1

1

5 6 1999 . 02 3.347960 NU3

6 4 2 757.78 0.431025 NUl

5 1 2406.15 9. 130832 NU3**-*

5 5 0 2406.15 9. 130832

9 5 4 1477 .31 4.762151 NU3*

3 1X 2 1772 .41 0. 597949 NU3*-''*-* 2 1 2 79.48 0.833333 NU 1-*^ 9 5 5 1474,99 n . m 949 5 NU3

7 7 X 1394.86 13.092131 NU3

7 7 0 1394.86 13.092131 X—^•W^t.X—JX NU3

1 1 6 5 2144. 12 5. 657103 NU3

2 1 1 95.17 1.500000 NU3

1 3 275.52 0.495229 NU3

7 5 782 . 40 5 . 91841

1

NUl

5 2 3 446 .50 3 . 44290

1

lMUl*«-

6 1 542.91 4.225862 NUl^*

5 2 3 446 . 50 1 . 147395 NU3-X8 6 2 1411 .68 8.307617 NU3**

1 0 1 23.79 1.500000 NU 1*

8 6 3 1411.65 8.307617 NU3**

9 3 1631 .41 0.576235 NUl

5 0 446 .71 0.016149 NU 1 8 4 4 1131.76 3.145152 NU3-*^

7 1 6 704.22 0.061078 NU3

8 1 7 882.93 0.049318 NU3

9 3 5 1282.92 7.165263 NU 1*

1 0 4 6 1616.51 0.293096 NUl

2 1 2 79.48 1 . 741385 NU 1^<-

2 1 2 79.48 1.500000 NU3-i^*

8 5 3 1255 .92 5.561462 NU3-**-

1 1 A A 2 1 42 - fi9 5.6571 03 NU3

X 2 79.48 0.833333 NU 1**

A 7 2433.85 4.929245 NU3

7 A•J 2 X ^ X 'w' • \J 9. 538170 NU3**

7 LJ

1X ± £- A, KJ % C. \J 9 . 53 8 1 70 NU 3**

1 0 6 4 1875.53 6.432643 NU3

6 1 5 542 .91 0.053326 NU3

6 2 4 602 .77 2.41 NU1 + 325.35 -J ^ J • V 0.01 10 53 NUl

4 222 . 06 2 . 047924 NUl

7 2 5 782.40 \J • V_/ Vi/ V-' I V_/ _/ NU3

8 A2 A"-J 982.91 6.368783 NUl

1 0 A 5 6 . 432643 NU3

7 n 7 (J u • ^ w 0.01 l^fiO NU 1 AO

11 542 .91 4.225862 NU 1

ft c; 1 2 5 5.16 5.561462 NU3*

3 1X 2 173.36 0. 597949 NU3^*-

9 4 5 1360.28 2 . 522255 NU3

A 2 315 79 2-167225 NU 1*

6 6 0 1045 . 07 11 . 108831 NU3**

6 6 1 1045 . 07 11 . 108831 NU3^^«-

50
LINE HALF

FREQUENCY STRENGTH WIDTH J'

^111 cm "

gm cm

~ cm~'nU tm1 1 1 1.

3707, 15 0.0530 0. 0909 5 3 2

3707. 16 0,2147 0. 1054 2 1 2

3707.46 160,7364 0.0909 5 3 2

3707. 50 0,3021 0.0588 7 5 3

3707.72 0,0562 0 .0886 5 2 3

3707.83 0,3283 0. 0763 5 2 3

3707.98 0,1007 0.0588 7 5 2

3708.21 0,1887 0 .0994 3 0 3

3708.25 9.8188 0 .0509 9 6 4

3708.34 0.1854 0.0939 3 2 2

3708.35 0.0276 0. 0793 1 2 5 7

3708.51 3.2732 0.0509 9 6 3

3708.96 3,0116 0.0802 6 4 2

3709.23 243.8891 0.0952 2 2 1 3709.42 2455.2679 0.1059 1 0 1 3709.68 0.8360 0.0546 6 5 1 3710.20 1.1225 0 .0642 10 5 6

3710.46 0.0214 0.0884 4 3 1 3710.69 1 1.0561 0.0487 8 6 3

3710.89 33.1701 0. 0487 8 6 2

3710.89 122.5898 0.0827 7 3 5 3711.09 580.2141 0. 1054 2 1 2

3711,32 0.6942 0.0486 5 5 0

3711.32 2 .0826 0.0486 5 5 1 3711,40 0. 1397 0 .0667 5 4 1 3711,72 0.5465 0.0863 1 0 4 6

3711.87 510.0087 0.0994 3 0 3

3712,20 4682 .0000 0.0989 1 1 1 3712 . 66 1 . 5409 0.1054 0 0 0

3712.80 2.1502 0.0750 8 3 6

3712.85 33.8205 0.0451 7 6 1 3712.85 101 .4617 0.0451 7 6 2

3713.15 0.1988 0.0892 3 3 1 3713.28 28 .0766 0.0886 5 2 3

3713.31 0.7199 0. 0694 8 3 5 3713.39 0.0542 0.0914 5 1 4

3713.43 5.1230 0.0887 9 4 5

3713.79 0.0615 0.0818 7 3 5

3714.02 0.0670 0.0961 4 0 4

3714.08 0.3306 0 . 0854 3 3 0

3714.26 0,0180 0.0614 8 5 3

3714.43 0.4330 0.0971 3 1 3

3714.53 1 .0415 0.0528 8 6 3

3714.77 92.5882 0 . 0408 6 6 1 3714.77 277.7646 0.0408 6 6 0

3715. 13 0.0177 0.0751 8 4 4

3715. 16 0.0559 0.0588 7 5 3

3715.48 0,1624 0.0620 9 4 6

3715.62 0.0187 0.0588 7 5 2

3715.73 0.3472 0.0502 8 6 2

3715.86 0.1982 0.0770 10 3 8

3716.01 0.2714 0.0829 5 3 3

3716.07 64.9813 0.0884 4 3 1 3716.19 13.7273 0.0633 9 5 5

J

1/Kq Kc t

1L BAND

cm"!

5 2 3 2053.98 3.442901 NUl^^-«-

1 0 1 23 . 79 1.500000 NUl^*

5 2 3 446.50 3.442901 NUl

7 5 2 1059.85 6.486001 NU3*

4 3 2 382.52 0.436045 NU 1^

4 4 0 488 . 13 0.002437 NU3

7 5 3 1059 .65 6.486001 NU3^^

2 1 2 79 .48 1 . 741385 NUl**

9 6 3 1631.41 7. 297946 NU3

3 1 3 142 . 28 1.297651 NU 1*

12 4 8 2205.65 9. 504415 NUl

9 6 4 1631.27 7, 297946 NU3

7 2 5 782 . 40 0.032449 NU3

2 1 2 79 .48 0.833333 NUl

2 0 2 70 .08 1.961754 NU3

6 5 2 888 .60 7. 626602 NU3*

10 5 5 1724,72 4.030316 NU3

4 2 2 1922.92 2. 167225 NUl***

8 6 2 1411.68 8. 307617 NU3

8 6 3 1411.65 8.307617 NU3

7 3 4 842 .38 1.781698 NU3

1 0 1 23.79 1 . 500000 NU 1 5 5 1 742 .10 9. 130832 NU3*

5 5 0 742 . 10 9.130832 NU3*

5 4 2 2251.71 5. 742440 NU3***

10 3 7 1538 .23 8.179783 NUl

2 1 2 79.48 1,741385 NUl

2 1 2 79 .48 1,500000 NU3

1 0 1 1618.55 1 , 000000 NU3***

7 4 3 931.22 0,519243 NUl

7 6 2 1216.20 9,538170 NU3

7 6 1 1216.20 9, 538170 NU3

4 0 4 222 . 06 0,004153 NU 1 4 3 2 382.52 0.436045 NUl

9 1 8 1079 . 07 0, 034132 NU3

5 0 5 1920.76 1,912338 NUl***

9 3 6 1282 .92 7, 165263 NU 1 8 0 8 744 .09 0,017472 NUl

3 1 3 1739.51 2,831638 NUl***

3 2 1 212. 15 1,092505 NUl*

8 5 4 1255.16 5, 561462 NU3**

3 1 2 173.36 0. 597949 NU3**

7 5 2 1059.85 5 . 144364 2NU2

6 6 0 1045 . 07 11.108831 NU3

6 6 1 1045.07 11.108831 NU3

8 4 5 . 2764.71 3. 145152 NU3***

7 5 2 1059.85 6.486001 NU3**

8 5 3 1255.92 0. 597432 NUl

7 5 3 1059.65 6.486001 NU3**

7 5 3 1059.65 5 . 142711 2NU2

9 4 5 1360.28 0. 409296 NUl

5 3 2 2130.50 2. 240000 NU3***

4 2 2 315 .79 2. 167225 NUl

9 5 4 1477.31 4.762151 NU3
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kc

cnn~i cm~i

gm cm-2

cm ' aim.

. _^ 9 3-J A 3716.58 92 .6790 0.0 939 3 2 2

3716.83 0.1610 0.0907 4 2 3

3716.87 9.3386 0.1054 0 0 0

3716.93 0.3314 0.0711 5 4 3

3716.98 0.32 87 0.0914 5 1 4

371 7-0? 0.01 70 0.0 583 1X 1X 1 1

0

0.0515 n . 0 546 5 5 2

0 . 1546 5 5 3717.71 0.03 39 0. 0879 A 3 4

3717.78 0 . 2663 0.0 999 C 1 2

3718.07 0 , 0440 n . 0607 9 4 6

3718. 14 0.2566 0.0760 9 3 7

3718.23 0.0160 0 . 0947 ^ 1 3

3718.36 0 .4456 0 . 0896 4 2 3

3718 . 42 0.0190 0.0848 7 2 5 3718.52 0. 5089 0. 1026 3 1 3

3718.60 0 .9759 0.0907 4 2 3

3718.64 0.0612 0.0854 3 3 n 3718.95 4.3541 0 . 0 894 8 4 4

3718.97 572.6216 0.0887 2 4

3719.39 1 .0003 0.071

1

\J 9 ^ 1 XX A 4 2

3 71 9.48 0 . 0 546 0.0854 3 3 n 3719.72 2.5369 0.0 667 5 4 2

3719,73 17.0275 0.0751 8 4 5 3719,95 0.1077 0.0830 3 3 1 3719,95 0.0635 0.0737 7 4 4

3719.96 0,05 54 0.0876 7 4 3

3719.96 1 ,6446 0.0 829 5 3 3

3720.02 0.0735 0.0 896 4 2 3

37?0 . 09 X1 6-1 \J % X 346 -J ^ \J 0-0614 8 5 4

3720-10 0.0360 0.0735 X1 7c~ 4 8

3720.12 0 . 8468 0.0 667 5 4 1 3720.3 5 0.1166 0.0 737 7 4 3

3720.37 0,2501 0.0800 4 3 2

3720-59 0 .0608 0.0914 w 9 \J y X ^ 5 1 4

3720.67 0.0248 0.0619 10 5

3721 .33 1 .9441 0.0605 4 4 1 372 1 . 39 5.8332 0.0605 4 4 0

3721 .51 43 .3543 0.0947 4 1 3

3721.62 0.3606 0.0829 3 2

377 1 .6? 4 . 65 64 0.0633 9 5 4

3771 - 86 51.4633 0 - 0 84R 7 2 5

3771 .88 48.68 59 0.0614 8 5 3

3722.19 1170.3233 0.0971 3 1 3

3777 .35 1 .9306 0,0758 3 3 1 3722.69 0 ,6443 0.0758 3 3 n 3722.77 0,75 57 0 . 0800 4 3 1 3722.8 2 1 5 1 , 0475 0.0588 7 5 3

3722.98 1,6144 0,0999 2 1 2

3723 .20 165,3169 0,0854 3 3 0

3773 .76 5 0.3551 0 . 0 58R 7 5 2

3723.35 3 .5672 0,0642 10 5 5

3123. 0.0110 0.0848 7 3 4

J" Kc E L BAND

9 2 7 1201.95 6.247031 NUl

3 1 3 142.28 1.297651 NUl

4 2 2 1922.92 1 .519518 NU3^-**

1 0 1 23 .79 1.000000 NU3*

6 4 2 757.78 4. 707057 NU3*

5 0 5 325.35 1.912338 NUl*

10 3 7 1538.23 0.016855 NU3

6 5 1 888 .63 7.626602 NU3*^«-

6 5 2 888 .60 7.626602 NUS*^-^

6 3 3 661 .56 1 .610000 NU3**

2 1 1 1693 .65 0.833333 NU3*->*

8 1 7 882.93 0.269351 2NU2

8 4 4 1 131 .76 0. 505247 NUl

3 2 2 206.30 0.835095 NU1*^«-

4 1 4 224.83 1 . 567300 NUl*

7 1 6 704.22 3. 983004 NUl**

2 0 2 70 .08 2. 156792 NUl*

4 2 2 315.79 1.519518 NU3*

3 2 1 212.15 1.092505 NUl**

8 3 5 1050.15 5.709388 NUl

5 2 3 446.50 1. 147395 NU3

6 4 3 756.75 4. 707057 NU3*

3 2 1 1819.34 1.092505 NUl***

5 4 1 610.35 5. 742440 NU3*

8 4 4 1131 .76 3,145152 NU3

3 2 2 206.30 1,035682 NUl*

7 4 3 931.22 3,870291 NU3**

7 3 4 842.38 4, 268667 NUl*

5 3 2 508 .81 2, 240000 NU3*

4 1 4 1821.61 1 , 567300 NUl***

8 5 3 1255.92 5, 561462 NU3

12 3 9 2105 .90 8,242761 NUl

5 4 2 610.12 5.742440 NU3*

7 4 4 927.77 3,870291 NU3*

4 3 1 2005.92 3,310000 NU3***

5 0 5 325.35 1,912338 NUl**

9 6 4 1631.27 0.586260 NUl

4 4 0 488 .13 7. 160948 NU3*

4 4 1 488. 10 7. 160948 NU3*

3 2 2 206.30 0.835095 NUl

4 2 3 300.35 1.848533 NUl*

9 5 5 1474.99 4.762151 NU3

7 1 6 704.22 3.983004 NUl

8 5 4 1255.16 5. 561462 NU3

3 1 2 173.36 0. 597949 NU3

3 3 0 1907.63 5.203793 NU3***

3 3 1 1907.47 5.203793 NU3***

4 3 2 2004.81 3.310000 NU3***

7 5 2 1059.85 6.486001 NU3

2 1 1 95.17 0.833333 NU3*

3 2 1 212.15 1 .092505 NUl

7 5 3 1059.65 6.486001 NU3

10 5 6 1718.77 4.030316 NU3

6 4 3 756.75 0.550367 NUl*

52
LINE HALF E" L BAND

FREQUENCY STRENGTH WIDTH

atm.

J' J" Kc

cm"'

UN 1 gm cm~2

3724,20 164.3495 0,0914 5 1 4 5 0 5 325.35 1.912338 NUl

3724.50 1.7277 0, 1054 0 0 0 1 0 1 23.79 1.000000 NU3^^<-

3724.62 0.0613 0,0711 6 4 3 6 4 2 757.78 4. 707057 NU3*^<-

3724.90 139.3240 0,0546 6 5 2 6 5 1 888.63 7.626602 NU3

3724.94 1.1515 0.0910 3 2 2 3 2 1 1819.34 2.151589 NU3***

3724.98 417.9811 0.0546 6 5 1 6 5 2 888.60 7.626602 NU3

3725.20 0.4062 0. 0961 4 0 4 3 1 3 142 .28 2.831638 NUl*

3725.40 0.0431 0.0879 4 2 2 5 0 5 325.35 0.023440 NU3*

3725.41 0.0909 0.0803 5 3 3 5 2 4 416.22 2.492169 NUl*

3725.44 0,2198 0.0976 4 1 4 3 0 3 1731.89 3.004990 NUl***

3725.66 91.5553 0.0829 6 3 4 6 3 3 661.56 1.610000 NU3-

3725.95 1.5155 0.0800 4 3 2 4 3 1 383.85 3.310000 NU3*

3726.05 0,0667 0.0829 4 3 2 4 2 3 300.35 1.848533 NUl**

3726.45 254.4680 0.1026 3 1 3 2 0 2 70.08 2. 156792 NUl

3726.50 222.7880 0.0896 4 2 3 4 1 4 224.83 1 . 567300 NUl

3726.62 347.1002 0.0486 5 5 0 5 5 1 742. 10 9.130832 NU3

3726.62 1041 .3007 0. 0486 5 5 1 5 5 0 742. 10 9. 130832 NU3

3727.00 0.1850 0.0711 6 4 2 6 4 3 756.75 4. 707057 NU3**

3727.01 17.8522 0.0854 4 3 1 5 1 4 399.46 0.028214 NU3

3727.37 0.4693 0.0667 5 4 2 5 4 1 610.35 5. 742440 NU3**

3727.73 0,3042 0.0829 5 3 3 5 3 2 508 .81 2.240000 NU3**

3727.74 171 .4775 0.0737 7 4 4 7 4 3 931.22 3.870291 NU3

3728.33 5.4781 0.0848 7 3 4 6 4 3 756.75 0.550367 NUl

3728.72 4.5800 0.0800 4 3 1 4 3 2 382.52 3. 310000 NU3*

3728.74 0.2604 0.0646 11 5 6 11 5 7 1985.83 3. 347960 NU3

3728.87 0.8541 0.0912 2 2 1 2 2 0 1743.47 3.269589 NU3***

3728.91 53.8748 0.0830 3 3 1 3 2 2 206.30 1 .035682 NUl

3728.95 0.0752 0.0961 4 0 4 3 1 3 142.28 2,831638 NUl**

3728.98 0*3597 0.0605 4 4 1 4 4 0 488 . 13 7, 160948 NU3**

3729.04 1.0791 0.0605 4 4 0 4 4 1 488 . 10 7. 160948 NU3**

3729.08 6.9788 0.0910 3 2 2 3 2 1 212.15 2. 151589 NU3*

3729. 13 0,5629 0.0829 5 3 2 5 3 3 504,00 2. 240000 NU3*

3729.26 0.0564 0.0637 9 3 6 10 1 9 1293,04 0.023266 NU3

3729.26 1.8787 0.1027 1 1 1 1 1 0 1640,51 1 . 500000 NU3***

3729.33 11,7012 0.0758 3 3 1 3 3 0 285,43 5.203793 NU3*

3729.47 0,0162 0.0855 4 1 3 3 3 0 285,43 0.007215 NU3*

3729.77 0,0168 0.0803 5 3 3 5 2 4 416.22 2.492169 NUl**

3729.80 3,9047 0.0758 3 3 0 3 3 1 285.23 5.203793 NU3*

3730.02 0,7482 0.0749 7 0 7 6 2 4 602.77 0.009797 NU3

3730.04 27,7032 0.0876 7 4 3 7 3 4 842 .38 4.268667 NUl

3730. 16 0,0978 0.0815 5 2 4 5 1 5 326.64 1.711792 NUl*

3730.49 0,1957 0.0600 10 4 7 9 5 4 1477.31 0. 720783 NUl

3730.49 180,3214 0.0829 4 3 2 4 2 3 300.35 1.848533 NUl

3730.68 0,2987 0.0999 2 1 2 2 1 1 95.17 0.833333 NU3**

3730.96 0,6472 0.0747 10 3 7 10 2 8 1438.00 5.910419 NUl

3731.33 0,0149 0.0922 4 0 4 3 2 1 1819.34 0.027572 NU3***

3731.38 2,5800 0.0912 2 2 0 2 2 1 1742 .28 3.269589 NU3***

3731.42 0,1640 0.0751 6 3 4 6 2 5 552.92 2. 963539 NUl*

3732. 13 4669,2922 0. 1054 0 0 0 1 0 1 23.79 1 .000000 NU3

3732.31 165,7268 0.0711 6 4 3 6 4 2 757.78 4. 707057 NU3

3732.70 203,1144 0.0961 4 0 4 3 1 3 142.28 2.831638 NUl

3732.82 1,3321 0.0976 4 1 4 3 0 3 136.77 3.004990 NUl*

3732.88 0,0161 0.0815 5 2 4 5 1 5 1922.86 1.711792 NUl***

3733.20 0,1847 0.0880 5 0 5 4 1 4 1821.61 3.911752 NUl***

53
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm~i cm~i cm ~~ ^

o m r- fx~\ — 2 y M 1 Ll M *- n tm

3733.26 0.0134 0.0759 8 2

3733.26 0.0154 0.0817 6 0

3733.63 0.2804 0.0800 4 3

3733.97 11.3858 0.1027 1 1 3734.09 0.0765 0.0945 2 2

3734. 13 45 .4466 0.0803 5 3

3734.23 5.1762 0.0912 2 2

3734.29 487.9030 0.0907 4 2

3734.61 500.1260 0.0711 6 4

3735.03 1268.4414 0.0667 5 4

3735.38 58.3012 0.0737 7 4

3735.41 423 .3935 0.0667 5 4

3735.51 822.3154 0.0829 5 3

3735.91 0.3965 0.0910 3 2

3736.08 0.1273 0.0558 9 6

3736.33 0,8473 0.0800 4 3

3736.63 972.0568 0.0605 4 4

3736.69 2916,5519 0.0605 4 4

3736.80 0.2464 0.0976 4 1 3736.81 1.2910 0.0910 3 2

3736.95 15.6361 0.0912 2 2

3736.98 2 .1647 0.0758 3 3

3737.27 0.0441 0.0653 13 4

3737.34 0.0200 0.0640 11 3

3737.44 0.7224 0.0758 3 3

3737.88 1 .0676 0. 1021 2 2

3737.97 0.1284 0.0639 12 5 3738.21 48.9070 0.0815 5 2 3738.24 0.1762 0. 1021 2 2

3738. 39 807.2323 0.0999 2 1 3739. 10 53 .7027 0.0751 8 4

3739. 13 0.0635 0.0900 5 1 3739.86 0.0126 0.0827 7 3

3739.98 6.6819 0.0759 8 2

3739.98 81 .9777 0.0751 6 3

3740.09 0.0167 0. 0840 6 4

3740. 37 50.4661 0.0840 6 4

3740.39 2 .4940 0.0792 6 2

3740.42 0.6447 0. 1027 1 1 3740. 79 666.0628 0.0976 4 1 3740.79 21 .5634 0.0879 4 2

3740.85 14.1716 0,0922 3 2

3741.32 757.7312 0,0800 4 3

3741.48 2.4032 0,0910 3 2

3741.64 2.1063 0, 1027 1 1 3741 .90 0.9575 0,0912 2 2

3742. 1

1

0.1975 0, 1021 2 2 3742.22 0.0142 0,0945 2 2

3742.37 8.1063 0,0855 4 1 3742.46 0.3214 0,0918 5 1 3742.76 0.8640 0,0792 5 4

3743.56 29.0700 0,0806 6 1 3743.95 2289.9859 0,0800 4 3

3744. 18 281.4220 0,0829 5 3

J" K E" L BAND

cm-i

6 8 1 7 882,93 3, 773034 NUl*

6 5 2 3 446.50 0.015393 NU3-^

2 4 3 1 383,85 3, 310000 NU3**

1 1 1 0 42 .37 1. 500000 NU3*

0 3 0 3 136.77 0.016142

3 5 2 4 416.22 2.492169 NUl

1 2 2 0 136. 17 3.269589 NU3*

3 4 2 2 315.79 1.519518 NU3

2 6 4 3 756.75 4. 707057 NU3

2 5 4 1 610.35 5. 742440 NU3

3 7 4 4 927,77 3.870291 NU3

1 5 4 2 610,12 5. 742440 NU3

3 5 3 2 508,81 2. 240000 NU3-

1 3 2 2 1813,81 2.151589 NU3***

4 8 5 3 1255.92 5.013867 2NU2

1 4 3 2 382.52 3. 310000 NU3**

1 4 4 0 488 . 13 7. 160948 NU3

0 4 4 1 488. 10 7. 160948 NU3

4 3 0 3 136.77 3. 004990 NU1*^<-

2 3 2 1 212. 15 2.151589 NU3*-«-

0 2 2 1 134.91 3.269589 NU3*

1 3 3 0 285.43 5.203793 NU3**

9 13 3 10 2414.73 8.21407 NUl

8 10 2 9 1293 .66 0. 316624 2NU2

0 3 3 1 285.23 5.203793 NU3**

1 1 1 0 42 .37 1. 500000 NUl*

7 12 5 8 2275 .44 2.746007 NU3

4 5 1 5 326.64 1.711792 NUl

1 1 1 0 1640.51 1. 500000 NUl***

2 2 1 1 95.17 0.833333 NU3

4 8 4 5 1122.72 3.145152 NU3

5 4 0 4 1817,50 3.972803 NUl***

4 7 3 5 2439,97 1 .430000 NU3***

6 8 1 7 882,93 3. 773034 NUl

4 6 2 5 552,92 2.963539 NUl

2 6 3 3 2282 , 59 9.42 NUl***

2 6 3 3 661 , 56 9,42 NU1 +

4 5 4 1 610,35 0,011274 NU3

0 1 1 1 1634,97 1 , 500000 NU3***

4 3 0 3 136,77 3,004990 NUl

2 5 0 5 325 ,35 0,023440 NU3

1 4 0 4 222,06 0,027572 NU3

2 4 3 1 383 ,85 3,310000 NU3-

1 3 2 2 206,30 2,151589 NU3*

1 1 1 0 42,37 1, 500000 NU3**

1 2 2 0 136, 17 3,269589 NU3**

1 1 1 0 42,37 1.500000 NUl**

0 3 0 3 136,77 0.016142 NU3**

3 3 3 0 285,43 0.007215 NU3

4 4 2 3 300,35 1.636916 NUl*

1 6 2 4 602 ,77 0.011274 NU3

5 6 0 6 446,71 1.852055 NUl

1 4 3 2 382,52 3, 310000 NU3-

2 5 3 3 504,00 2,240000 NU3-

54
LINE HALF

Kq FREQUENCY STRENGTH WIDTH J' K

cm~' cm"' cm"'

qm cnn~2 atm.

3744. 55 3489.4356 0.0910 3 2 2

3744. 64 5850.5869 0.0758 3 3 1 3745.09 1952.3806 0,0758 3 3 0

3745. 52 139,8683 0,0720 6 4 3

3745.55 1 0 . 1844 0, 0893 6 2 4

3746. 12 4.8467 0.0746 9 4 5 3746.34 533.7904 0.1021 2 2 1 3746. 86 0.1023 0.0787 5 4 1 3747.23 16.9013 0.0696 7 4 4

3747,41 309.9884 0.0787 5 u 1 3747.43 0.3847 0.0900 5 1 5

3747.74 0.0899 0. 0922 4 0 4

3747.82 0.0437 0.0457 10 _^ 8

3748. 17 0.0311 0.0710 6 2 5 3748.28 13.8194 0.0682 7 3 5

3748.31 0.5214 0.0655 11 3 8

3748.49 2.4978 0. 0794 9 5 4

3748.65 0.0562 0.0949 2 2 0

3748.75 0.0387 0.0583 10 3 7

3748.99 7 . 7443 0.0817 6 0 6

3749.20 160.6755 0.0918 5 1 4

3749.31 5692 .9022 C. 1027 1 1 1 3749. 57 2588.0843 0.0912 2 2 1 3750.26 12.2782 0.0 6 56 8 4 5 3750.29 0.0364 0.0603 8 3 6

3750.35 38.2258 0.0945 2 2 0

3750.60 0.0471 0.0760 6 0 6

3750.63 0,0458 0.0720 4 4 0

3750.88 3.1891 0.0907 4 2 2

3750.95 138.9137 0.0720 4 4 0

3751. 10 0.8717 0.0999 2 1 1 3751.48 559.7738 0.0880 5 0 5 3752.14 83.9324 0.0710 6 2 5

3752.21 7818 .0682 0.0912 2 2 0

3752.53 420.3516 0.0689 4 4 1 3752.84 151.8258 0.0949 2 2 0

3753.54 0.1430 0.0779 6 1 6

3753.64 1 .6436 0.0563 10 5 6

3753.73 105.4296 0.0719 5 4 2 3754. 18 0.0346 0.0704 7 5 2

3754.61 5.2830 0.0999 2 1 1 3754.68 12 ,7948 0.0945 3 0 3

3754.71 0.0866 0.0671 7 1 6

3754.80 2.8489 0.0855 3 3 0

3755. 13 1.5863 0.0600 9 4 6

3755.15 0.3050 0.0984 3 2 2

3755.40 192.3580 0.0900 5 1 5 3755.92 0.0758 0.0827 7 3 4

3756.61 1201 .5765 0.0910 3 2 1 3757.63 2 .0594 0.0756 8 5 3

3757.69 0 . 1234 0.0586 10 6 5 3758.13 16 .9430 0.0645 6 6 1 3758.32 0.0213 0.0567 9 6 4

3758.33 0. 5899 0.0907 4 2 2

J" Kc E" L BAND

cm"'

c X 212.15 7.1515ft9 Nl 1^

-> 0 285 .43 5. 203793 NU3

3 3 1 285.23 5. 203793 NU3

6 3 4 648 .97 8.16 NU1 +

5 3 3 504.00 0.863547 NU 1 9 4 6 1 340 .89 2,522255 NU3

1 1 0 42.37 1 , 500000 NU 1 5 3 2 2130.50 8 , 97

7 3 5 816.72 6,84 NU1 +

5 3 2 508.81 8,97 MU1 +

4 0 4 222 . 06 3,972803 NU

3 2 1 212.15 0.027572 NU3-K9 0 9 920.18 0 . 106449 2NU2

5 J. 447 , 24 1.783035 NU i*-*;- 7 2 A 709.60 3_J .• 273499 C- I ^ '-r J y NU

1

1

1

2 9 ] 690 . 70 5 . 642326 NU 1 9 4 5 1360.28 5.113359 NU 1 1 1 1 37.13 1,244 747 NU l*-«-

1

1

1 1 0 1524.87 0.016855 NU3

5 2 3 446 .50 0,015393 NU3

4 2 3 300.35 1 , 638916 NUl

1 ] 0 42.37 1,500000 NU3

2 2 0 136.17 3.269589 NU3

8 3 6 1 006 .12 4. 264036 NUl

8 2 7 885.62 3.456295 NU 1-^

3 0 3 136.77 0.016142 NU3

5 1 5 1922.86 4 . 95 8 549 |\|Ul^^-«-*

3 1 2005,92 6.45 NU 1***

4 2 3 300.35 1.519518 NU3*

4 3 1 383.85 6 .45 NU1 +

2 1 2 1677 . 08 0,833333 NU3***

4 1 4 224.83 3,911752 NU 1 6 6 447 . 24 1.783035 NUl

2 2 1 134.91 3,269589 NU3

4 3 2 382,52 6.46 NU 1 +

1 1 1 37.13 1 . 244747 NU 1 5 0 5 1920.76 4.1^ • 979001 ' y \y \J X NU l*-!<-* 1 0 7 1581.34 10.08 NU1 +

5 3 3 504.00 8.92 NU1 +

7 4 3 931.22 4.12 NUl*

2 1 2 79.48 0. 833333 NU3*

2 2 0 136.17 0.016142 NU3

7 0 7 586.26 1.838288 NUl*

4 1 3 275.52 0.007215 NU3

9 3 7 1216.27 4.734521 NUl

2 1X 95.17 1 .666667 NUl*

4 0 4 222.06 3 .972803 NU 1 7 3 5 816.72 1 . 430000 NU3*

3 2 2 206.30 2. 151589 NU3

8 4 4 1131.76 4.012859 NUl

9 5 4 1477.31 4.857731 2NU2

Au 4 648 .97 1 f 5 . 8 0 2NU2 + 10 4 7 1581 .34 0.012276 NU3

4 2 3 300.35 1.519518 NU3**

55
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm-1

gm cm~2

cm""'

atm.

3758,40 18,2093 0,0603 8 3 6

3758.45 0,0285 0,0601 7 2 6

3758. 51 0,0897 0,0515 11 5 7

3758.63 7,3609 0,0646 9 2 7

3759.08 295,1506 0,0829 6 3 3

3759.79 1953 ,3406 0.1027 1 1 0

3760. 15 0,5201 0. 1043 1 0 1 3760.37 7.5790 0.0879 5 0 5

3760.84 0,2856 0.0760 6 0 6

3761 . 33 0,0530 0.0525 IP 4 7

3761 . 51 1.2792 0.0851 8 3 5 3761 .64 1 ,6062 0,0536 10 4 7

3762. 18 43,3012 0,0671 7 1 6

3762 .20 0,9774 0.0999 2 1 1 3762 , 47 44,9303 0,0922 4 0 4

3762.48 0.8664 0,0779 6 1 6

3762.75 0.0579 0.0468 12 5 8

3763.03 0.0141 0.0827 7 3 4

3763. 13 0.1327 0.0661 11 6 5

3763.69 152.5244 0.0984 3 2 2

3764. 16 3.1523 0. 1043 1 0 1 3764.48 2 .4607 0.0749 6 2 4

3764. 58 17.2987 0,0704 7 5 2

3764.75 0.0528 0,0760 6 0 6

3765 . 10 0.4514 0,0887 5 2 3

3765.79 1594.5383 0.0907 4 2 2

3766.09 6.5014 0,0854 5 1 4

3766.38 0.0968 0,0735 9 3 6

3766.39 14.2643 0,0601 7 2 6

3766.48 0.1603 0,0779 6 1 6

3766.71 10 .9598 0,0620 8 5 4

3766.78 0,0487 0,0557 12 3 9

3766.78 0,1530 0,0971 3 1 2

3766.80 0,0938 0,0631 7 0 7

3766 .87 0,2810 0.0694 9 1 8

3767.00 0,0985 0.0843 6 1 5

3767 . 40 0,8589 0.0600 9 5 5 3768.01 7,8283 0.0624 7 5 3

3768.09 0,0314 0.0642 7 1 7

3768.09 0 ,0400 0.0845 6 1 5 3768,26 0,4062 0.0583 8 6 3

3768.66 142,8230 0.0760 6 0 6

3768.93 12,7448 0.0646 6 5 1 3769.22 0,1212 0.0955 4 2 3

3769.33 0,7348 0.0955 4 2 3

3769.47 0,9269 0.0971 3 1 2

3769. 52 2 ,3651 0.0529 9 3 7

3769.80 2641 ,4699 0.0999 2 1 1 3769.95 47,2035 0.0607 6 5 2

3770. 15 37,8850 0.0827 7 3 4

3770.21 1,1541 0.0802 7 2 5 3770.48 433,2210 0.0779 6 1 6

3771,11 0,0954 0.0594 8 4 5

3771,20 0,3417 0.0721 6 5 1

J E L BAND

cm-1

8 2 7 885.62 3,456295 NUl

7 1 7 586 , 48 1 ,816721 NU 1*

1

1

4 8 1843,02 6.097371 NU 1 9 1 8 1079 , 07 3. 674255 NU 1 6 3 4 648 , 97 1.610000 NU3-

1 1 1 37,13 1 . 500000 NU3

0 0 0 1594,73 1 .000000 NU3**-=<-

4 2 2 315,79 0.023440 NU3

5 1 5 326,64 4.958549 NUl*

9 1 8 1079 ,07 0,284777 2NU2

7 4 4 927,77 0,898681 NU 1 10 3 8 1446 ,16 5,051335 NUl

7 0 7 586,26 1,838288 NUl

2 1 2 79,48 0,833333 MU3**

3 2 1 212,15 0,027572 NU3

5 0 5 325,35 4, 979001 NUl*

1 2 4 9 2124,98 6 . 558344 NUl

7 3 5 816,72 1 . 430000 NU3**

1

1

5 6 1999 , 02 6. 009423 NUl

2 1 1 95,17 1 . 666667 NUl

0 0 0 0 , 1 . 000000 NU3*

7 0 7 586,26 0.009797 NU3

7 4 3 931,22 4.12 NU1 +

5 1 5 326 , 64 4. 958549 NUl**

5 2 4 416,22 1.147395 NU3*

4 2 3 300,35 1 . 519518 NU3

4 3 1 383.85 0.028214 NU3

8 5 3 1255 .92 0.032937 NU3

7 1 7 586 .48 1.816721 NUl

5 0 5 325.35 4.979001 NUl**

8 4 5 1122.72 6.79 NU1 + 12 2 10 1960.22 5 . 509361 NU 1 3 1 3 1739.51 0. 597949 NU3***

6 1 6 2042 .77 5.983681 NUl***

8 3 5 1050. 15 0. 034132 NU3

5 2 4 416.22 2.671788 NU 1*

9 4 6 1 340 .89 4.736397 NUl

7 4 4 927 .77 5.49 NU1 +

6 0 6 2041 .76 5 . 990506 NUl***

5 3 2 508 .81 0.053826 NU3*

8 3 6 1006 .12 1 .52 2N.U2 +

5 1 5 326.64 4. 958549 NUl

6 4 2 757.78 3.82 NU1 +

3 1 2 1772 .41 1.970843 NUl***

3 1 2 173.36 1.970843 NUl*

3 1 3 142.28 0. 597949 NU3*

9 2 8 1080.38 3. 554957 NUl

2 1 2 79 . 48 0.833333 NU3

6 4 3 756.75 4.69 NU1 +

7 3 5 816.72 1.430000 NU3-

6 4 2 757.78 0 . 032449 NU3

5 0 5 325.35 4. 979001 NUl

9 2 8 1080,38 0.013441 NU3

7 3 4 842,38 0.004886 NU3

56
LINE HALF

FREQUENCY STRENGTH WIDTH J'

gm cm

r-rr\ — 1 0 tm. 3771.45 78.2781 0.0580 5 5 0

3771.68 26.1273 0.0566 5 5 1 3771.83 0.5831 0. 1C43 1 0 1 3772.10 0.0132 0.0542 8 1 7

3772.41 0.1322 0.0620 10 6 4

3772.42 0.0835 0.0887 5 2 3

3772.46 0.0890 0.0798 8 3 5 3773.28 0.0156 0.0607 6 5 2

3773.34 0.6647 0.0642 7 4 4

3773.40 0.0998 0.0544 9 4 6

3773.65 0.1359 0.0955 4 2 3

3773.84 0.0394 0.0503 8 2 7

3773.92 0.0294 0.0486 12 6 7

3773.97 2,8476 0.0726 10 4 6

3774.05 49.2429 0.0843 6 1 5

3774.69 0.0258 0.0580 5 5 0

3774.96 0.0893 0.0785 10 4 6

3775.57 0.0428 0.0515 11 6 6

3775.65 0.0352 0.0734 7 1 6

3775.96 0.8407 0. 0534 10 2 8

3776.46 0.6509 0,0989 2 1 2

3776.55 0.2623 0,0649 7 5 3

3777.01 0.1714 0,0971 3 1 2

3777.02 0.5527 0.0961 3 2 1 3777.08 0.5683 0.0631 7 0 7

3777.11 26.1526 0.0859 7 2 5

3777.44 0.0912 0.0961 3 2 1 3777.97 367.3966 0.0955 4 2 3

3778.22 0.4141 0.0529 10 6 5

3778.29 1.2356 0.0763 4 4 0

3778.67 0.0116 0.0466 6 6 1 3779.05 1.1050 0.0587 9 6 3

3779.50 1576.1857 0.1043 1 0 1 3779.74 225.6980 0.0887 5 2 3

3779.76 6.5911 0.0542 8 1 7

3780.25 0.0302 0.0927 5 2 4

3780.49 0.3911 0.0691 6 4 3

3780.60 0.1828 0.0927 5 2 4

3780.85 0.1187 0.0427 12 4 9

3781.02 3.9448 0.0989 2 1 2

3781.04 0.1051 0.0631 7 0 7

3781.15 0.1023 0.0961 3 2 1 3781.25 0.3731 0.0534 9 6 4

3781.48 0.0128 0.0577 8 6 3

3781.68 0.0352 0.0642 7 1 7

3781.78 19,7042 0.0503 8 2 7

3781.90 3 .4583 0.0754 8 1 7

3781.97 20,0055 0.0845 6 1 5

3782.27 2.7335 0. 1059 2 0 2

3782.48 2.4819 0.0458 10 3 8

3782.70 0,0613 0.0810 8 5 4

3782.81 0.0550 0.0523 8 1 8

3783.38 0.5625 0.0847 6 2 4

3783.65 0.8520 0.0553 8 6 2

I" J

1/Kq 1/Kc F"C.

1L RAND

cm"i

5 4 1 610,35 3,74 NU1 +

5 4 2 610,12 3,74 NU 1 +

0 0 0 0 , 1,000000 NU3''<"'«' o0 0

0 "lit r\C\

1 44 .09 1 0 0 (~1 ~7 "7 Q 1,839 / ^0 Ml 11 ii- NU i 10 5 5 1724,72 4,974368 Ml IT NU 1 5 2 4 416.22 1 , 147395 NU 3*''^ o0 3 6 1 006 .12 1 , i^^b^oi

6 4 3 4,69 Ml IT AS- ^ ^

QO 2

-7 U,Uii / 9j

1

0

2 9 1293 .66 0, 013637 Ml 10 NU3

3 1 2 173,36 1 , 970843 NU 1**

8 1 8 744 , 16 1,833129 NUl^*-

12 5 8 2275 ,44 6,631337 NU 1 1

0

4 7 1581,36 1 , 530000 NU3-

5 2 4 416,22 2,671788 Ml IT NU 1 5 4 1 2251,86 3,74 Ml t 1 J(. J' y

9 5 5 1474 ,99 0. 959644 Mill NU 1 1

1

5 7 1985,83 5.799382 Mill NU 1 6 2 5 2161,30 3. 799063 Ml IT Jt. Jt. .1'

1

0

1 9 1293 , 04 3 . 6468 1

5

M 1 1 T NU 1

1 1 1 16 34,9

/

1.500000

8 3 6 1006,12 0.00 8488 NU3

3 1 3 142,28 0 . 59 7949 NU 3*-5<- 2 1 2 79 , 48 0. 925282 NU 1*

6 1 6 447 ,24 5.983681 M 1 1 T ^ NU 1^

6 3 4 648 , 9 ' 1.512999 MM! NU 1 2 1 2 1677,08 0.925282 Ml IT ^ J'

3 1 2 173,36 1.970843 M 1 1 T NU 1

1 0 5 6 1718 ,77 4.913223 NU 1 5 2 3 446 ,50 0 . 002437 NU3

6 5 2 808 ,60 1.11160^ Ml IT ^1. NU 1 5 4 1477,31 4. 017231 Mill NU 1

(J 0 0 0 ,

T r\ r\ r\ t\ r\ r\ 1.000000 Ml 1 O NU3

5 2 4 416,22 1 . 147395 Ml 1 0 NU3

Q8 0 0 ^ 44 , 09 T Q 0 "7 "7 Q 1.839778 Mill NU 1 4 1 3 1875 ,49 2 . 444582 NU l**'*^- 7 2 6 709,60 0.008618 NU3

4 1 3 2 5 , 5 2

0 /././COT 2 . 444582 NU 1^

12 3 1

0

1962,55 5.350112 Mill NU 1 1 1 1 37,13 1.500000 NU3*

6 1 6 447 , 24 C (O 0 0 ^ 1 5,983681 NU i**

•5*1 1 c"7 0 /. Q

^ 9 , 4c) 0,92!3282

Q c

!? 14 (4,99 4, 001691 Mill

9 4 6 1 340 ,89 0,006585 Ml to NU3

6 0 6 446 ,71 5 , 990506 NU 1**

8 1 8 744, 16 1,833129 h 1 1 1 T NU 1 7 3 '+ 842,38 0 , 0493 1

8

NU3

5 3 2 508,81 0,053826 Ml to NU3

1 0 1 1618,53 1,961754 Nil 1 0 ^Ji. Ji.

1 0 2 9 1 <i 93 , 66 3,605841 1 1 T NU 1

-77 2 5 782 ,40 0,074366 T M 1 10 2NU2

7 0 7 2180,65 7,000291 NU I***-

6 2 5 552,92 0,939536 NU3*

8 5 3 1255,92 3,077042 NUl

707-944 O - 64 - 5 57
LINE HALF DbAlNJU A MH

FREQUENCY STRENGTH WIDTH J'

ill J Kc E L

cnn"i cnri~l gm cm~2 atm.

3783.90 0.2562 0. 0680 7 2 5 8 0 8 744.09 0.006703 NU3

378A-. 02 0.0254 0.0470 13 3 10 13 2 11 2246.98 5.73352 NUl

3784.36 2 .5674 0.0527 8 6 3 8 5 4 1255. 16 3.073714 NUl

3784. 56 463.4236 0.0971 3 1 2 3 1 3 142.28 0.597949 NU3

3785.01 284.1359 0.0631 7 0 7 6 1 6 447.24 5.983681 NUl

'3785.28 276.3516 0.0961 3 2 1 2 1 2 79.48 0.925282 NUl

3785.69 95 .0855 0.0642 7 1 7 6 0 6 446.71 5.990506 NUl

3786.01 16.5667 0. 1059 2 0 2 1 0 1 23 .79 1.961754 NU3*

3786.26 44.5172 0.0798 8 3 5 8 3 6 1006. 12 1.436963 NU3

3786.68 0.2526 0.0934 4 1 3 4 1 4 1821.61 0.495229 NU3***

3786.90 4.7126 0.0515 7 6 1 7 5 2 1059.85 2. 119964 NUl

3787. 10 1 .5705 0.0506 7 6 2 7 5 3 1059.65 2. 119434 NUl

3787.40 3 .5309 0.0801 7 1 6 6 3 3 661 .56 0.061078 NU3

3787.61 0.0263 0.0459 12 7 6 12 6 7 2433.85 5.917211 NUl

3787.67 1 .9075 0. 1037 2 1 1 1 1 0 1640.51 1. 500000 NU3***

3787.97 1.5311 0.0934 4 1 3 4 1 4 224.83 0.495229 NU3-K3788.02 0.0165 0.0443 9 1 8 9 0 9 920.18 1.844131 NUl*

3788.06 0,2133 0.0734 7 1 6 6 2 5 552.92 3. 799063 NU1^<-

3788.72 0.7298 0.0989 2 1 2 1 1 1 37.13 1.500000 NU3**-

3788.78 0 ,2689 0.0688 11 4 7 11 4 8 1843 .02 1. 701473 NU3

3789.24 1 .9386 0.0469 6 6 0 6 5 1 888.63 1. 111654 NUl

3789.27 5.8155 0.0466 6 6 1 6 5 2 888 .60 1. 111607 NUl

3789.33 91 .4180 0.0927 5 2 4 4 1 3 275.52 2.444582 NUl

3789.92 0,3605 0.0842 3 3 1 2 2 0 136. 17 2.394805 NUl*

3790.38 0.0445 0.0488 11 7 4 11 6 5 2144.12 4.999181 NUl

3790.60 0.1040 0.0847 6 2 4 6 2 5 552.92 0.939536 NU3**

3791.20 0.3789 0.0873 6 2 5 5 1 4 399.46 3. 129447 NUl*

3791.37 1 .0755 0.0840 3 3 0 2 2 1 134.91 2.366160 NUl*

3791.44 0.0154 0.0442 11 2 9 10 1 10 1114,56 0.097873 2NU2

3791 . 57 11.5607 0. 1037 2 1 1 1 1 0 42 ,37 1. 500000 NU3*

3791.79 0.0395 0.0734 7 1 6 6 2 5 552,92 3. 799063 NUl**

3791.79 0.0148 0.0473 11 7 5 11 6 6 2142,69 4.990193 NUl

3791.87 0.7954 0.0442 11 2 9 11 1 10 1524.87 3.646421 NUl

3792.30 0.1976 0.0410 8 7 1 7 6 2 1216.20 6.263414 2NU2

3792.30 0.5929 0.0410 8 7 2 7 6 1 1216.20 6. 263444 2NU2

3792.46 1.4121 0.0722 5 4 2 6 2 5 552 .92 0.004724 NU3

3792.71 0.3332 0.0523 8 1 8 7 0 7 586.26 7.000291 NUl*

3792.73 0.0943 0.0520 8 0 8 7 1 7 586.48 5.95 NUl*

3793.72 3 .0648 0. 1059 2 0 2 1 0 1 23.79 1.961754 NU3**

3793.83 2.9731 0.0784 8 2 6 7 4 3 931.22 0.065935 NU3

3794.48 0.0667 0.0842 3 3 1 2 2 0 136. 17 2.394805 NUl**

3795. 14 0.0483 0.0475 10 7 3 10 6 4 1875.53 4.061130 NUl

3795.47 0.2833 0.0934 4 1 3 4 1 4 224.83 0.495229 NU3**

3795.48 2.3034 0.0820 9 3 6 8 4 5 1122.72 1.416234 NUl

3795. 52 106 .6507 0.0734 7 1 6 6 2 5 552.92 3.799063 iMUl

3795.67 0. 1447 0.0463 10 7 4 10 6 5 1875.00 4.058996 NUl

3795.77 0.2644 0.0406 11 3 9 11 2 10 1525.13 3.632655 NUl

3795.85 8.2511 0.0443 9 1 8 9 0 9 920. 18 1.844131 NUl

3795.90 0. 1990 0.0840 3 3 0 2 2 1 134.91 2.366160 NUl**

3796.09 2 .8097 0.0984 3 1 3 2 1 2 1677.08 2.653490 NU3***

3796.43 1972.3763 0.0989 2 1 2 1 1 1 37.13 1. 500000 NU3

3796.86 2.7480 0.0430 9 2 8 9 1 9 920.21 1 .842036 NUl

3796.95 0.0287 0.0436 9 0 9 8 1 8 2337.70 8.007087 NUl***

3797.08 2.3801 0.0757 5 3 3 6 1 6 447.24 0.004689 NU3

58
LINE HALF

FREQUENCY STRENGTH WIDTH J' K

gm cm "2 otm.

3797.29 0,0159 0.0628 7 6 1 3797.82 281.2435 0.0847 6 2 4

3798.49 0,4030 0.0459 9 7 2

3798, 53 1,0581 0.0809 4 3 2

3798. 58 3,7621 0.0907 3 3 0

3798.60 0.0131 0.0781 7 2 6

3798,63 0.1343 0.0454 9 7 3

3799. 04 180.2308 0.0842 3 3 1 3799.24 2.1387 0. 1037 2 1 1 3799.85 7 .9446 0.0760 8 4 4

3799.92 189.4512 0.0873 6 2 5 3800.44 537.7475 0.0840 3 3 0

3800. 5.8 17.0284 0. 0984 3 1 3

3800.74 0.4287 0.0682 6 3 4

3800.77 47. 1439 0.0520 8 0 8

3800.79 166.5854 0.0523 8 1 8

3801 .43 8283 .3461 0.1059 2 0 2

3802.00 1.3395 0,0915 3 2 2

3802.31 0.0369 0,0669 11 2 9

3802.97 765.5725 0.0934 4 1 3

3803. 51 0,8768 0.0948 3 2 2

3803.76 0,3817 0. 0401 7 7 1 3803.76 1 ,1452 0. 0401 7 7 0

3804. 11 0.0770 0.0782 7 2 5

3804.87 0.2422 0.0605 8 2 6

3805.22 7.4254 0. 1010 3 0 3

3805.24 2.3152 0.0837 3 3 1 3805.62 0.0146 0.0781 7 2 6

3805.82 0.1163 0.0766 11 4 7

3806 .03 4,4716 0.0740 9 3 6

3806.19 6.0791 0.0793 8 2 6

3806,25 0,4469 0.0907 3 2 1 3806,33 0,0483 0.0573 7 6 2

3806,37 8,1183 0.0915 3 2 2

3806,91 5780,3612 0. 1037 2 1 1 3807,45 0,1737 0.0436 9 0 9

3807,54 0.0579 0.0437 9 1 9

3808,00 0.5153 0.0763 9 2 7

3808,04 0,0184 0.0422 11 8 3

3808 ,26 0.2284 0. 0368 12 3 10

3808, 30 0,2844 0.0863 5 1 4

3808. 32 3.1503 0. 0984 3 1 3

3808. 54 0,3006 0.0729 4 4 1 3808.58 0,1438 0.0633 12 4 8

3808,98 0,0304 0.0687 5 4 1 3809,09 0 ,0469 0.0863 5 1 4

3809,11 0.5633 0.0620 7 3 5 3809,46 0.7202 0.0868 4 3 2

3809.80 2 .3407 0.0892 4 3 1 3809.96 39.5794 0.0781 7 2 6

3810.81 0.4963 0.0718 10 2 8

3811.20 0.0141 0.0410 10 8 2

3811,20 0.0423 0.0408 10 8 3

3811,23 1 .0476 0.0382 10 1 9

i" Kq E L BAND

cm-1

8 4 4 1131 .76 0.002886 NU3

6 2 5 552.92 0.939536 NU3

9 6 3 1631.41 3. 1 16419 NUl

5 1 5 326.64 0.003420 NU3

3 0 3 136 .77 0.016715 NUl

6 1 5 2146.28 4.008107 NUl-^*^^-

9 6 4 1631.27 3. 116005 NUl

2 2 0 136.17 2. 394805 NUl

1 1 0 42 .37 1 . 500000 NU3*->«-

7 1 7 586.48 10.90 2NU2 +

5 1 4 399 .46 3. 129447 NUl

2 2 1 134.91 2.366160 NUl

2 1 2 79 .48 2.653490 NU3*

7 1 7 586 ,48 0.005077 NU3

7 1 7 586,48 5.95 NUl7 0 7 586,26 7.000291 NUl

1 0 1 23 .79 1 .961754 NU3

2 2 1 1742.28 1.666667 NU3^-^^'^

10 4 6 1616.51 0.075083 NU3

4 1 4 224.83 0.495229 NU3

3 0 3 136.77 0. 181744 NU3^^

7 6 2 1216.20 1. 119792 NUl

7 6 1 1216.20 1.119797 NUl

7 2 6 709 .60 0.838975 NU3*

9 0 9 920. 18 0.005067 NU3

2 0 2 70.08 2. 880004 NU3^

4 1 4 224.83 0.001497 NU3

6 1 5 542 .91 4. 008107 NUl^-

10 5 6 1718.77 1.370216 NUl

9 3 7 1216 .27 1.235624 NU3

7 3 5 816.72 2.422109 NUl

2 2 0 1743.47 1 .676022 (MU3-''^**

8 4 5 1 122 . 72 0.002778 NU3

2 2 1 134.91 1 . 666667 NU3^«-

1 1 0 42.37 1.500000 NU3

8 1 8 744. 16 8.007087 NUl*

8 0 8 744.09 8.007851 NU1^<-

8 4 4 1131 .76 0.092972 NU3

1

1

7 4 2321 .94 4. 105208 NUl

12 2 11 1774.74 3. 648229 NUl

5 1 5 326,64 0.456689 NU3*

2 1 2 79,48 2.653490 NU3**

5 2 4 416.22 0.001517 NU3

12 4 9 2124.98 1.508618 NU3

6 1 6 447 . 24 0.000636 NUl

5 1 5 1922 .86 0.456689 NU3**-=^

8 1

8' 744. 16 0.004883 NU3

3 2 1 212.15 2. 320352 NUl*

4 0 4 222.06 0.047652 NUl

6 1 5 542 .91 4.008107 NUl

9 4 5 1360.28 0.093773 NU3

10 7 3 2054.40 3.150851 NUl

10 7 4 2054,40 3.150801 NUl

10 0 10 1114.55 1 .848326 NUl

59
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm-1 cm-1

gm cm -2 atm.

3811.25 0.0142 0.0782 7 2 5 3811.45 2.7080 0.0907 3 2 1 3811.51 0.0321 0.0436 9 0 9

3811.55 0,0134 0.0381 10 1 10

3811.60 0.0107 0.0437 9 1 9

3811.72 0.1622 0.0948 3 2 2

3811.79 0.3152 0.0916 4 2 3

3811.82 3.1420 0.0378 10 2 9

3812.39 0. 1447 0.0948 3 2 2

3812.64 0.8666 0 .0986 3 1 2

3812.68 0.0106 0.0507 9 1 8

3812.99 1 .3738 0.1010 3 0 3

3813.17 0.1326 0.0646 8 2 7

3813.50 0.9625 0.0948 4 1 4

3814.07 0 .1332 0.0868 4 3 2

3814.08 1 .5019 0.0915 3 2 2

3814.25 2 1 .1080 0,0613 8 1 7

3814.61 0.1164 0.0385 9 8 1 3815.21 0.0388 0.0385 9 8 2

3815.57 86.8369 0.0436 9 0 9

3815.66 82 .0644 0.0977 2 2 1 3815.67 28.9611 0.0437 9 1 9

3816.07 8514.1759 0. 0984 3 1 3

3817.44 0.0245 0.0646 8 2 7

3817 . 52 0,0733 0.0444 9 7 3

3817 . 55 0.2198 0.0443 9 7 2

3818.12 0,0589 0,0364 8 8 0

3818.12 0,1767 0,0364 8 8 1 3818.34 0,0313 0,0970 4 2 2

3818.39 38,4497 0,0782 7 2 5 3818.69 360,1188 0,0868 4 3 2 3818 . 78 3 ,0435 0.0960 4 0 4

3819.09 0,5010 0,0907 3 2 1 3819.43 5,8335 0, 0948 4 1 4

3819.93 438.3722 0.0948 3 2 2

3820.77 3712.7214 0,1010 3 0 3

3821.72 66 .2925 0.0646 8 2 7

3821.79 4059 . 1468 0.0915 3 2 2

3822.17 18.4455 0.0960 4 0 4

3822.40 0.0643 0.0507 9 1 8

3823.30 142.2114 0.0863 5 1 4

3823.97 0.9717 0.0986 3 1 2

3824.05 0.5723 0.0846 5 2 4

3824.30 94,8028 0.0970 4 2 2

3824. 54 1,1771 0.0774 4 3 2

3824. 85 0,0208 0.0698 9 2 7

3825. 10 0 ,0926 0,0689 8 2 6

3825.16 0,1438 0,0892 5 3 3

3825.21 0,0252 0,0543 9 2 7

3825.56 160.1007 0,0861 4 3 1 3825.70 3 .4366 0,0784 4 3 1 3825.94 0.5450 0.0903 4 2 3

3826.09 0.0151 0.0381 10 1 10

3826.39 1 .0898 0.0348 11 1 10

J Kc c"E L BAND

7 2 6 709 . 60 0.838975 NU3**

2 2 0 136 , 17 1 .676022 NU3*

8 1 8 744 .16 8. 007087 NU 1**

9 0 9 2512,36 9.013676

8 0 8 744 , 09 8.007851 NUl**

3 0 3 136,77 0. 181744 NU3**

4 0 4 222 , 06 0. 299684 NU3*

10 1 10 1114,56 1 .847651 NUl

3 0 3 1731,89 0. 181744 NU3***

2 1 1 1693,65 2 . 645088 NU3*-'<--K- 8 2 7 2495 , 18 5.987889 NUl***

2 0 2 70 , 08 2.880004 NU3**

7 1 6 704.22 4.996649 NUl*

3 1 3 1739 .51 3.713893 NU3***

3 2 1 212.15 2 . 320352 NUl**

2 2 1 134.91 1.666667 NU3**

7 2 6 709 .60 4.913532 NUl

9 7 2 1810.63 2.165395 NUl

9 7 3 1810.63 2.165389 NUl

8 1 8 744.16 8.00 7087 NUl

2 0 2 70.08 0 . 063744 NU3

8 0 8 744 . 09 8.007851 NU 1 2 1 2 79 .48 2. 653490 NU3

7 1 6 704 .22 4. 996649 NUl**

8 6 2 1411 .68 6. 142105 2NU2

8 6 3 1411 .65 6. 141896 2NU2

8 7 1 1590.74 1.126216 NUl

8 7 2 1 590 . 74 1 . 126215 NU 1 3 1 3 1739.51 1.29 NUl***

7 2 6 709 . 60 0.838975 NU3

3 2 1 212.15 2.320352 NUl

3 0 3 1731 .89 3. 805784 NU3***

2 2 0 136.17 1.676022 NU3**

3 1 3 142.28 3.713893 NU3*

3 0 3 136. 77 0. 181744 NU3

2 0 2 70 . 08 2.880004 NU3

7 1 6 704.22 4. 996649 NUl

2 2 1 134,91 1.666667 NU3

3 0 3 136,77 3.805784 NU3*

8 2 7 885,62 5.987889 NUl*

5 1 5 326,64 0.456689 NU3

2 1 1 95,17 2 . 645088 NU3**

5 0 5 325,35 0.303000 NU3*

3 1 3 142,28 1.29 NU1 +

3 3 1 285,23 1.530000 NU3*

8 3 6 1006,12 3 . 529968 NUl*

8 2 7 885,62 0. 807542 NU3*

4 2 2 315.79 2. 324407 NUl*

10 0 10 1114.55 0. 004155 NU3

3 2 2 206 . 30 3 . 00 NU1 +

3 3 0 285 .43 1 . 490000 NU3*

3 2 2 1813.81 2. 890000 NU3***

9 0 9 920. 18 9,013676 NUl**

11 0 11 1327.14 1.851910 NUl

60
LINE HALF

FREQUENCY STRENGTH WIDTH J' K rm ""1 rrn ~" 1 gm cm -2 atm.

3826.74 1353.9804 0, 0907 3 2 1 3827.22 1 .0792 0 ,0948 4 1 4

3827.29 0.2311 0,0857 5 3 3

3827.46 3 .9394 0,0671 10 3 7

3828.02 157,6210 0,0916 4 2 3

3828.07 0.4002 0,0752 10 3 7

3828.29 3.3028 0, 0903 4 2 3

3828.42 0.4631 0,0773 6 1 5

3828,61 67.3233 0,0880 5 3 2

3828.91 0.0945 0 , 0 846 5 2 4

3829.78 0.0247 0,0574 13 4 9

3829.86 0.0266 0,0892 5 3 3

3830.01 3.4125 0, 0960 4 0 4

3830. 16 13.5642 0,0381 10 0 1 0

3830.20 40 .6942 0,0381 10 1 10

3830.41 32.1513 0,0507 9 1 8

3831 . 58 10.3849 0,0698 9 2 7

3831.67 2626.1743 0.0986 3 1 2

3831.96 2.4478 0.0872 5 1 5

3832.24 0.2177 0. 0774 i\ 3 2

3832.26 0.0172 0.0689 8 2 6

3832.33 0.1486 0. 0743 7 3 5

3833.37 0.6358 0.0784 4 3 1 3833.39 0.2513 0.0633 5 4 2

3833.46 0.0838 0.0638 5 4 1 3833.71 1 .6711 0.0914 4 2 2

3833.96 0.1032 0.0747 6 2 5

3834. 14 10.9281 0.0539 9 2 8

3834. 56 71.9165 0,0892 5 3 3

3835.02 2916.7265 0.0948 4 1 4

3835.72 0.0134 0.0813 6 3 4

3835.88 2,4530 0.0957 4 1 3

3835.98 0.0857 0.0773 6 1 5

3836.03 0,6110 0.0903 4 2 3

3836.07 0.0427 0.0857 5 3 3

3836.39 14,8350 0,0872 5 1 5

3836.81 0.2376 0,0896 6 3 4

3836.90 0.0169 0,034 14 3 12

3837.85 9222.7358 0, 0960 4 0 4

3838.35 5 .0508 0,0887 5 0 5

3838.72 10.1279 0,0914 4 2 2

3838.80 0.0939 0,0 860 3 3 1 3838.88 0.0289 0 , 0444 10 2 9

3838.94 14.8661 0,0957 4 1 3

3839.43 46.3159 0,0689 8 2 6

3839. 94 588,5700 0 ,0774 4 3 2

3840. 12 286,1386 0 ,0846 5 2 4

3840.59 0,1143 0,0331 1 2 1 1

1

3840.69 0,3429 0,0331 12 2 11

3841 .04 1718,3218 0 ,0784 4 3 1 3841 .60 0,0440 0 ,0896 6 3 4

3841 .68 1 ,2546 0,0875 5 2 4

3841.70 0,6429 0,0803 5 3 3

3841.80 0,0270 0,0663 8 3 6

J" E" L BAND

/-«nr\ — 1 LI 11

2 2 0 136,17 1.676022 NU3

3 1 3 142,28 3.713893 NU3*^<-

5 1 4 399 .46 0.177000 NU3*

10 3 8 1446. 16 1.142576 NU3

4 0 4 222 .06 0.299684 NU3

9 4 6 1340.89 2. 171641 NUl

3 2 2 206.30 2.890000 NU3*

6 1 6 447. 24 0.450603 NU3*

5 0 5 325.35 0.762 NU1 +

5 0 5 1920.76 0.303000 NU3-^**

13 4 10 2426,22 1. 549000 NU3

4 2 2 315 .79 2.324407 NUl**

3 0 3 136.77 3.805784 NU3**

9 1 9 920.21 9.013420 NUl

9 0 9 920. 18 9.013676 NUl

8 2 7 885,62 5.987889 NUl

8 3 6 1006 ,12 3. 529968 NUl

2 1 1 95 . 17 2.645088 NU3

4 1 4 1821.61 4.737042 NU3***

3 3 1 285.23 1. 530000 NU3**

8 2 7 885.62 0. 807542 NU3**

7 1 6 704.22 0. 522000 NU3*

3 3 0 285.43 1.490000 NU3**

4 4 1 2129.63 1,810924 NU3***

4 4 0 2129.65 1,810956 NU3***

3 2 1 1819 .34 3, 033776 NU3***

6 0 6 446 .71 0, 299000 NU3*

8 1 7 882.93 6,019178 NUl

4 2 2 315.79 2, 324407 NUl

3 1 3 142.28 3,713893 NU3

6 1 5 542,91 0.339000 NU3**

3 1 2 1772,41 3.667441 NU3***

6 1 6 447,24 0.450603 NU3**

3 2 2 206,30 2.890000 NU3**

5 1 4 399 ,46 0. 177000 NU3**

4 1 4 224,83 4. 737042 NU3*

5 2 3 446,50 2.452523 NUl*

14 2 13 2327.90 3.76386 NUl

3 0 3 136.77 3.805784 NU3

4 0 4 222 .06 4.769122 NU3*

3 2 1 212.15 3.033776 NU3*

3 1 2 173 .36 0.023148 NU3*

9 1 8 1079.07 7.043661 NUl*

3 1 2 173,36 3. 667441 NU3*

8 2 7 885,62 0.807542 NU3

3 3 1 285,23 1. 530000 NU3-

5 0 5 325,35 0.303000 NU3-

12 0 12 1557.91 1.854934 NUl

12 1 12 1557.91 1.854861 NUl

3 3 0 285.43 1.490000 NU3-

5 2 3 446.50 2.452523 NUl**

4 2 3 1907.99 3.530000 NU3***

4 3 2 2004.81 2, 730000 NU3***

8 1 7 882.93 0,691047 NU3*

61
LINE HALF

FREQUENCY STRENGTH WIDTH J' K, cnn~^ cm-1

am cm -2 otm.

3841 .87 1.5227 0.0633 5 4 2

3841 .91 0.0191 0. 0747 6 2 5

3842.00 0.5076 0.0638 5 4 1 3843. 54 231 .5447 0 .0773 6 1 5

3843.78 165 1 .4006 0.0903 4 2 3

3844.23 2.7445 0.0872 5 1 5 3844.31 36.1015 0.0813 6 3 4

3844. 37 17,1819 0 .0349 1

1

0 1

1

3844.38 5.7274 0.0349 1

1

1 1

1

3844. 86 115 .5386 0.0857 5 3 3

3845 .30 0. 1888 0.0826 5 3 2

3845 .37 0.0408 0.0881 7 3 5 3845.40 4.7726 0.0431 10 1 9

3845. 55 0.0241 0.0516 6 5 2

3845. 59 0.0721 0.0516 6 5 1 3845.61 0,0381 0.0857 5 3 3

3846.22 0.9344 0.0887 5 0 5 3846.35 1.8736 0.0914 4 2 2

3846.36 3.8963 0.0803 5 3 3

3846.40 118.7903 0.0896 6 3 4

3846.69 2.7503 0.0957 4 1 3

3846 .70 0.3282 0.0994 2 2 0

3846 .78 0.0245 0 .0743 7 3 5 3847.14 0.0783 0.0654 7 1 6

3847.31 1^ .^440 0 , 0444 10 2 9

3847 .75 0,0174 0.0860 3 3 1 3848.63 0.3784 0 .0596 1

1

3 8

3843 .89 0 ,2144 0.0674 4 4 1 3848.90 0.5974 0 .0764 6 1 6

3849.05 74.3308 0 .0743 7 3 5 3849.07 1 . 1444 0.0826 5 3 2 3849.08 0.0656 0.0 66 5 4 4 0

3849. 53 7.6040 0. 0875 5 2 4

3849. 57 198.6771 0.0665 4 0

3849.62 649.673e> 0.0674 4 4 1 3849.65 31.1338 0.0871 4 3 2 3849.86 51 .6049 0 .0747 6 2 5 3850.25 0.2312 0.0636 7 2 6

3850.36 1 .3076 0.0775 6 0 6

3852.07 7417.5214 0.0872 5 1 5

3852.73 1 .6180 0.0590 10 2 8

3853.14 0.3522 0. 0884 5 3 2

3853 .42 3.6207 0.0 764 6 1 6

3853.61 1067.1312 0.0884 5 3 2

3853.99 5063.9614 0.0914 4 2 2 3854. 10 2525 .4405 0.0887 5 0 5 3854.30 10.9552 0.0775 6 0 6

3854.44 7433.0627 0.0957 4 1 3

3855.01 0 .0607 0.0994 2 2 0

3855 . 1 1 20.3797 0.0881 7 3 5 3855.11 0.0541 0 .0994 2 2 0

3855.47 0 .0345 0.0 333 1 3 2 12

3855.93 0.0161 0.0430 7 6 2 3856.00 0.1457 0.0516 6 5 2

J" Kc E" L BAND

cm~'

4 4 1 488 . 10 1.810924 NU3^

6 0 6 446 .71 0. 299000 NU3^(-^

4 4 0 488. 13 1.810956 NU3*

6 1 6 447.24 0.450603 NU3

3 2 2 206.30 2.890000 NU3-

4 1 4 224.83 4. 737042 NU3**

6 1 5 542 .91 0.339000 NU3-

10 1 10 1114.56 10.018153 NUl

10 0 10 1114.55 10.018239 NUl

5 1 4 399.46 0. 177000 NU3-

4 3 1 2005.92 2.420000 NU3***

6 2 4 602 .77 2.751216 NUl*

9 2 8 1080.38 7.032041 NUl

5 5 1 2406. 15 1.845180 NU3***

5 5 0 2406. 15 1.845182 NU3***

5 1 4 2000.90 0. 177000 NU3***

4 0 4 222 .06 4.769122 NU3**

3 2 1 212.15 3.033776 NU3-K-X4 3 2 382 . 52 2.730000 NU3*

5 2 3 446.50 2.452523 NUl

3 1 2 173 .36 3,667441 NU3-X-*

1 0 1 23 .79 0,038246 NU3*

7 1 6 2309.74 0.522000 NU3-=^**

7 1 7 586 .48 0.456726 NU3*

9 1 8 1079.07 7.0^3661 NUl

3 1 2 173.36 0.023148 NU3-«-*

1

1

3 9 1695.03 1 . 122765 NU3

3 3 0 1907,63 5.89 NUl***

5 1 5 1922.86 5,744669 NU3***

7 1 6 704.22 0. 522000 NU3-

4 3 1 383.85 2.420000 NU3*

3 3 1 1907 .47 5.49 NUl***

4 2 3 300.35 3.530000 NU3*

3 3 1 285.23 5.49 NU1 +

3 3 0 285.43 5.89 NU1 +

4 1 3 275.52 0.076900 NU3-

6 0 6 446.71 0.299000 NU3-

7 0 7 586.26 0.448059 NU3*

5 0 5 1920.76 5.755360 NU3***

4 1 4 224.83 4. 737042 NU3

9 3 7 1216.27 4. 706625 NUl

4 2 3 1907.99 10.59 NUl***

5 1 5 326.64 5..744669 NU3*

4 2 3 300.35 10.59 NU1 +

3 2 1 212.15 3.033776 NU3

4 0 4 222.06 4.769122 NU3

5 0 5 325.35 5.755360 NU3*

3 1 2 173.36 3.667441 NU3

1 0 1 23.79 0.038246 NU3**

6 2 4 602 .77 2.751216 NUl

1 0 1 1618.55 0. 038246 NU3***

13 1 13 1806.78 1.90640 NUl

6 6 1 2734.00 1.869458 NU3***

5 5 1 742 .10 1.845180 NU3*

62
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm ""^ cm ~ ^ nm rm ~ 2 Vf III \,/ 1 1 1 atm.

3856.05 0.4372 0.0516 6 5 3856.^6 0.6187 0.0926 5 1 3856.52 0.0847 0.0679 6 4

3856.70 0.2117 0.0826. 5 3

3856.71 46.9431 0. 0860 3 3

3856.76 268.3014 0.0834 5 4

3857.28 761 .3661 0.0633 5 4

3857.32 1 .4067 0.0875 5 2

3857.^0 253.7719 0.0638 5 4

3857.^8 0.2539 0.0699 6 4

3857.67 0.5327 0.0674 11 3

3857.67 6.5393 0.0332 12 1 3858.05 2 .1800 0.0332 12 0

3858.10 13 .4536 0.0663 8 3

3858.18 0.0427 0.0636 7 2

3858.74 3.7502 0.0926 5 1 3859.02 6.3714 0. 0800 6 4

3859.28 4 .9618 0.0840 4 4

3859.38 5 .9083 0.0606 9 2

3859.87 5.6605 0.0378 11 1 3860.44 0.0381 0.0636 7 2

3860.44 0.4683 0,0920 5 2

3860.66 1 .9004 0,0385 11 2

3861.31 0.6698 0,0764 6 1 3861 .47 19.4285 0. 0865 6 3

3861 .62 29,5843 0.0832 8 3

3861 .80 1948 ,1717 0.0803 5 3

3862.22 2,0267 0.0775 6 0

3862.48 39,1902 0.0654 7 1 3863.33 164.1211 0.0994 2 2

3863.71 0.0270 0.0516 6 5

3863.76 0.0809 0.0516 6 5

3863.80 0. 1548 0.0797 6 3

3864.33 572.2053 0.0826 5 3

3864.68 1.5832 0.0818 6 2

3864.74 0.0110 0.0657 10 3

3864,85 2.8384 0.0920 5 2

3865. 11 7.4267 0.0694 9 4

3865.12 3801 .9877 0.0875 5 2

3865.67 1.5388 0.0699 6 4

3865 .83 0.3867 0.0649 7 0

3865 .84 0.2932 0.0351 8 8

3865.84 0.0977 0.0351 8 8

3866.12 115.5784 0.0636 7 2

3866.58 0,6938 0.0926 5 1 3866.67 1 ,0017 0.0620 10 4

3866.99 4.4486 0.0754 9 3

3867.64 0.2765 0.0509 12 3

3867.71 0.9382 0.0797 6 3

3867.84 0.0260 0.032 14 2

3867.94 0.0160 0.0803 6 4

3868.20 7.4799 0.0756 7 4

3868.50 0.0652 0.0565 7 5 3868.53 0.0326 0.0430 7 6

1/ I" 1/ IL

R A MR

cm-1

1 5 5 0 742 . 10 1 . 845 182 NU3^

4 4 1 3 1875 .49 4.60 1931 NU3*^-"-

3 5 4 2 2251.71 3 . 35 1648 NU3-'-i--«--^ 2 4 3 1 383.85 2 . 420000 NU3-"--^

1 3 1 2 173.36 0,023148 NU3

1 5 1 4 399.46 4,37 NU 1 +

2 4 4 1 488.10 1,810924 NU 3 4 4 2 3 300.35 3 , 530000 NU3*-^

1 4 4 0 488.13 1,810956 NU3

2 5 4 1 2251.86 3.352166 l\IU3-«--«-*

8 1 0 4 7 1581 . 34 3 . 178818 NU 1 12 1

1

0 1

1

1327,14 11.021891 NUl

12 1 1 1 1

1

1327 , 14 11 .021861 NU 1 6 8 1 7 882,93 0. 69 1047 NU3

6 7 0 7 586,26 0. 448059 NU3 - ^

4 4 1 3 275,52 4. 601931 NU3^

2 6 1 5 542,91 0.637 NU1 +

0 4 1 3 275,52 0. 1303 NU1 +

7 9 2 8 1080,38 0.813942 NU3

10 10 2 9 1293,66 8 . 058917 NU 1 6 7 0 7 2180,65 0.448059 NU3*^^

3 4 2 2 1922 ,92 4.253846 NU3^->^-«- 10 1 0 1 9 1293 , 04 8.063213 NU 1 6 5 1 5 326,64 5 . 744669 N U 3 *

3 6 0 6 446 ,71 1.20 NU1 +

6 7 2 5 782 , 40 3 .262769 NUl

3 4 3 2 382,52 2.730000 NU3-

6 5 0 5 325,35 5.755360 N U 3

^- 6 7 1 7 586 ,48 0. 456726 NU3

0 1 0 1 23,79 0.038246 NU3

2 5 5 1 742 .10 1.845180 NU3-^-«-

1 5 5 0 742 .10 1 . 845182 N U 3

''^ -i^- 4 5 3 3 2126.41 3.600000 IM U 3

*<''<

2 4 3 1 383.85 2. 420000 NU3-

5 5 2 4 416.22 3 . 920000 NU 3-*^

8 9 2 7 1201.95 4.932263 NU 1*

3 4 2 2 315.79 4.253846 NU3*

6 9 2 7 1201.95 0. 624317 NU3

4 4 2 3 300 .35 3. 530000 NU3-

2 5 4 1 610.35 3.352166 NU3*

7 6 0 6 2041 ,76 6.749914 N U 3 *

1 7 7 0 1394,86 7. 402783 2NU2

0 7 7 1 1 394,86 7. 402783 2NU2

6 7 0 7 586,26 0. 448059 NU3

4 4 1 3 275,52 4. 60 193

1

NU3-«-^

7 10 2 8, 1438,00 0.828214 NU3

7 8 2 6 982,91 4. 004 942 NUl

9 1 2 3 10 1962 ,55 1 . 142616 NU3

4 5 3 3 504,00 3.600000 NU3^i13 14 1 14 2073 ,66 1 . 90878 NU 1 3 6 2 4 602 , 77 0. 100806 NU3-^

3 7 1 6 704. 22 0.557 NU1 +

3 6 5 2 2552.85 3.450020 NU3^^^*

1 6 6 0 1045 .07 1 . 869458 NU3*

63
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq K, cm~i cm ' gm cm"

2

i cm"i

atm.

3868 . 53 0.0977 n\j m. 0430 \j ^ -J ^1 7 A 2

3868.58 4.7672 0 , 0747 8 4 5

3868.62 0.0218 0.0569 7 5 2

3869.20 18 10 .3455 0 .0764 6 1 6

3869.82 7 .0093 0.0642 7 1 7

3869.86 16.9154 0.0 570 9 3 7

3870.14 5477.5779 0,0775 6 0 6

3870.58 1.9171 0 ,0494 1

1

2 9

3870.97 185.6067 0,0962 5 2 3

3871 .09 0.7449 0,0324 1

3

1 1 3

3871.09 2 .2347 0.0324 TX 3-J 0 1

3

3871.43 72.8685 0,0516 6 5 2

3871 .48 218 .6085 0,0516 6 5 1 3871 .80 0.3440 0,0861 6 3 3

3872.26 0 .0949 0.0679 6 4 3

3872.34 0.0203 0 .0547 8 1 7

3872.51 0.2928 0.0818 6 2 5 3872,51 0.5251 0.0920 5 2 3

3872 .55 0 .1700 0.0719 5 1 3872 .78 0.9988 0 . 0 546 1

1

8

3873.34 0.2847 0.0699 6 2

3873.37 0.6742 0.0350 1 2 1 1

1

3873.70 515.2017 0,0719 4 1 3873.73 2.0230 0,0350 1 7 2 1

1

3873.80 1.1966 0,0872 6 1 5 3873.88 236.4411 0 , 0742 5 4 2

3874. 19 5,5187 0,0657 10 3 8

3874.42 1875. 1260 0,0926 5 1 4

3875.42 7,2518 0,0872 6 1 5

3876.25 0,0181 0,0430 7 6 2

3876.33 0.2483 0,0971 3 2 1 3876 . 46 0.0886 0,0834 5 4 1 3876 . 56 21. 1764 0,0791 7 4 4

3876.85 0.0415 0,0576 1

2

8

3877.43 6.2732 0,0516 10 2 8

3877.61 0.0498 0,0521 13 5 9

3877.75 1.2967 0, 0642 7 1 7

3878. 13 0.4336 0 ,0649 7 0 7

3878. 53 0.0130 0,0469 8 6 2

3878.64 0.3954 0,0565 7 5 3

3878.87 0.1318 0,0 569 7 5 2

3879.43 0,1735 0,0 700 7 4 4

3879.44 0,0410 n . 0 79 7 4 2 3879.79 0,6045 n . 0 734 7 2 A

3879.97 256,6825 0,0679 6 4 3

3880.12 54,6477 0. 0547 8 1 7

3880.17 1419,2277 0.0920 5 2 3

3880.35 79 1,6073 0.0818 6 2 5

3881.01 769 ,3965 0.0699 6 4 2

3881.28 0,6656 0,0 535 8 0 8

3881.61 0,1054 0,047 7 1 2 4 9

3881.66 0,0462 0,0451 9 2 8

3881.76 0,0106 0,032 15 1 14

3881.81 18,1225 0,0531 8 2 7

J" Kc E L BAND

cm"!

6 6 1 1045,07 1,869458 NU3*

8 2 6 982,91 0,402567 NU3

6 5 1 2552,67 3,450058 NU3***

5 1 5 326,64 5, 744669 NU3

6 1 6 447,24 6,746361 NU3*

9 1 8 1079,07 0,769552 NU3

5 0 5 325,35 5,755360 NU3

10 3 8 1446 , 16 5,859437 NUl

4 1 4 224.83 1,257 NU1 + 12 0 12 1557.91 11,99676 NUl

12 1 12 1557.91 11,99672 NUl

5 5 1 742 . 10 1,845180 NU3

5 5 0 742 . 10 1,845182 NU3

5 3 2 2130.50 2,720000 NU3***

5 4 2 610.12 3,351648 NU3**

8 1 8 744. 16 0,464983 NU3**

5 2 4 416.22 3,920000 NU3**

4 2 2 315.79 4,253846 NU3*^-

4 3 2 2004.81 7,67 NUl***

1

1

2 9 1690.70 0,981559 NU3

5 4 1 610.35 3,352166 NU3**

11 2 10 1525.13 9,076485 NUl

4 3 2 382.52 7,67 NU1 + 11 1 10 1524,87 9,078065 NUl

5 1 4 2000,90 5,488405 NU3^*^<-

4 3 1 383.85 10,63 NU1 +

9 2 7 1201.95 4,932263 NUl

4 1 3 275.52 4,601931 NU3

5 1 4 399.46 5,488405 NU3*

6 6 1 1045.07 1,869458 NU3**

2 0 2 70.08 0.094498 NU3*

5 1 4 2000.90 4. 37 NUl***

7 2 5 782 .40 0.218314 NU3

12 3 9 2105.90 0.855326 NU3

10 2 9 1293.66 0. 834303 NU3

13 3 10 2414.73 1.031690 NU3

6 1 6 447.24 6. 746361 NU3**

6 0 6 446.71 6.749914 NU3**

7 6 1 2905 .42 3. 522866 NU3***

6 5 2 888.60 3.450020 NU3*

6 5 1 888 .63 3.450058 NU3*

6 4 3 2398.39 4.735129 NU3***

5 2 3 446.50 0.039164 NU3*

6 2 5 2161 .30 5.960000 NU3***

5 4 2 610.12 3. 351648 NU3

8 1 8 744. 16 0.464983 NU3

4 2 2 315.79 4. 253846 NU3

5 2 4 416.22 3.920000 NU3-

5 4 1 610,35 3. 352166 NU3

7 0 7 2180,65 7. 747248 NU3***

12 2 10 1960,22 1.085478 NU3

9 0 9 920, 18 0.471417 NU3*

15 0 15 2358 ,44 1.91083 NUl

8 0 8 744,09 0.462205 NU3

64
LINE HALF

BAND FREQUENCY STRENGTH WIDTH J' Kc J" Kc E" L

gm cm~^ otm.

3882.00 0.0576 0,0748 7 4 3 6 4 2 2399. 17 4. 739627 NU3-**-**

3882.88 2 .0675 0,0491 10 3 8 10 1 9 1293. 04 0.818434 NU3

3882.90 0.6787 0,0547 11 3 9 10 2 8 1438 ,00 5. 954956 NUl

3883.22 469.0807 0,0797 6 3 4 5 3 3 504.00 3.600000 NU3-

3883.37 1 .3416 0.0872 6 1 5 5 1 4 399.46 5. 488405 NU3*^

3883.42 0.1167 0.0527 5 5 1 4 4 0 488 .13 4.397010 NUl*

3883.45 0.3502 0.0525 5 5 0 4 4 1 488. 10 4,396748 NUl-«-

3883.60 3.6637 0.0734 7 2 6 6 2 5 552 .92 5,960000 NU3*

3883.98 0.0662 0. 0605 12 3 9 1

1

4 8 1843 . 02 4,355455 NUl

3883.98 16.2910 0,0430 7 6 1 6 6 0 1045.07 1,869458 NU3

3883.98 48.8730 0,0430 7 6 2 6 6 1 1045.07 1,869458 NU3

3884.08 2 .0845 0.0861 6 3 3 5 3 2 508.81 2.720000 NU3*

3884.20 0.0541 0.0862 4 3 1 4 1 4 224.83 0.017070 NU3*

3884. 58 0 ,0460 0.0971 3 2 1 2 0 2 70.08 0.094498 NU3**

3884.75 0.0410 0.0971 3 2 1 2 0 2 1664.97 0.094498 NU3***

3884.82 0,3211 0.0771 7 3 5 6 3 4 2271 .70 5. 110000 NU3***

3884.92 0,2374 0.032 14 0 14 13 1 13 1806.78 12,99955 NUl

3884. 92 0,7116 0.032 14 1 14 13 0 13 1806.78 12.99957 NUl

3885.37 0.9264 0.0917 6 2 4 5 2 3 2053.98 5.358633 NU3**^i3885.68 543 .9519 0,0800 6 4 3 5 3 2 508.81 15.18 NU1 + 3885.68 3504.6611 0,0642 7 1 7 6 1 6 447.24 6. 746361 NU3

3885.94 4.0338 0,0535 8 0 8 7 0 7 586.26 7.747248 NU3*

3886.08 1172.0190 0.0649 7 0 7 6 0 6 446.71 6. 749914 NU3

3886.47 0.6388 0.0332 13 1 12 12 2 11 1774.74 9.99731 NUl

3886.65 0.2130 0.0331 13 2 12 12 1 11 1774.60 9. 99954 NUl

3886.77 1.0514 0,0700 7 4 4 6 4 3 756.75 4.735129 NU3*

3887.32 8,0240 0,0803 6 4 3 6 2 4 602 .77 0. 100806 NU3

3888.04 6,7224 0,0870 3 3 0 3 1 3 142 .28 0.008443 NU3

3888.54 0,0216 0.0527 5 5 1 4 4 0 488 .13 4.397010 NUl**

3888.57 0,0648 0,0525 5 5 0 4 4 1 488. 10 4. 396748 NUl**

3888.68 1 .9460 0.0771 7 3 5 6 3 4 648 .97 5. 110000 NU3*

3888.76 0.2275 0.0785 7 1 6 6 1 5 2146.28 6.391209 NU3***

3888.77 5.6151 0,0917 6 2 4 5 2 3 446.50 5.358633 NU3*

3889.97 1.3791 0.0785 7 1 6 6 1 5 542 .91 6.391209 NU3*

3890. 12 0.3492 0.0748 7 4 3 6 4 2 757.78 4.739627 NU3*

3891.32 3625,9114 0.0872 6 1 5 5 1 4 399.46 5.488405 NU3

3891.66 0,3857 0.0861 6 3 3 5 3 2 508 .81 2. 720000 NU3**

3891.96 256,0173 0,0887 6 3 3 5 2 4 416.22 13.47 NU1 + 3892.30 0.6720 0,0454 12 3 10 11 2 9 1690.70 7.003088 NUl

3892.83 124.1187 0.0971 3 2 1 2 0 2 70.08 0.094498 NU3

3893.67 58 .3632 0.0527 5 5 1 4 4 0 488 . 13 4.397010 NUl

3893.69 0.6812 0,0444 11 2 9 1

1

2 10 1525.13 0.856092 NU3

3893.70 175.1005 0,0525 5 5 0 4 4 1 488. 10 4.396748 NUl

3893.76 0,2484 0.0532 8 1 8 7 1 7 586 .48 7.746063 NU3**

3893.92 0.7463 0.0535 8 0 8 7 0 7 586.26 7.747248 NU3**

3894.07 11,7787 0.0915 4 3 2 3 0 3 136.77 0.051049 NUl

3894.07 197.6637 0.0565 7 5 3 6 5 2 888 .60 3.450020 NU3

3894.28 65.8922 0.0569 7 5 2 6 5 1 888.63 3.450058 NU3

3894.49 0.1945 0.0700 7 4 4 6 4 3 756.75 4.735129 NU3**

3895.14 2.8823 0.0380 8 7 2 7 7 1 1394.86 1.887603 NU3

3895.14 8 .6468 0.0380 8 7 1 7 7 0 1394.86 1.887603 NU3

3896.27 0.0460 0.0755 6 4 2 5 3 3 2126.41 11.35 NUl***

3896.33 0.3424 0. 0446 9 1 9 8 1 8 2337 .70 8. 745235 NU3***

3896.40 2.0316 0.0427 11 3 9 11 1 10 1524.87 0.850512 NU3

65
LINE HALF

FREQUENCY STRENGTH WIDTH J' Ka

cnn~i

gm cm ~ 2 atm.

3895 . 46 0.1142 0.0447 9 0

3896.49 0.3600 0.0771 7 3

3896 .50 1 .0388 0.0917 6 2 3896 . 64 0.1131 0.0633 8 2 3896.69 0.2760 0.0694 10 5

3896.31 7.7064 0.0458 9 1 3896.81 0.0177 0.0397 10 1 3896. 90 0.0193 0.0527 5 5 3696. 92 0.0578 0.0525 5 5 3897.24 0.0778 0,032 15 1 3897.24 0 .1921 0,032 15 0

-3897.24 0.1054 0,0885 7 3

3897 .56 23.0795 0.0451 9 2

3897.93 139.3042 0.0755 6 4

3898.01 0.2552 0.0785 7 1 3898.29 214.0639 0.0725 6 6

3898.82 5.8341 0.0845 7 3

3898.82 0.0301 0.0692 5 4

3898.88 20.4906 0.0792 5 4

3899.24 1042.2919 0.0861 6 3

3899. 46 1831.8316 0.0734 7 2

3900. 35 0.6856 0.0633 8 2

3900.60 0.0070 0.0496 9 6

3900.95 0.0801 0.0594 8 5 3901.21 2.0752 0.0446 9 1 3901.25 0.6921 0.0447 9 0

3901.33 0.0123 0.0407 9 7

3901.64 27.0726 0.0862 4 3

3901.74 671 .4213 0.0532 8 1 3901.91 2016.9288 0.0535 8 0

3902.21 525 .6870 0.0700 7 4

3902.39 41.0263 0.0834 7 4

3903.35 4.7486 0.0662 6 6

3903.46 0,0858 0.0852 8 4

3903.90 2 ,1279 0.0670 8 1 3904.24 2807.5183 0.0917 6 2

3904. 30 972.9716 0.0771 7 3

3905.06 0.4026 0.0354 9 8

3905.06 1 .2079 0.0354 9 8

3905.10 0.0713 0.0656 6 4

3905.37 174.6112 0.0748 7 4

3906.05 689.5227 0.0785 7 1 3906, 17 13 .1418 0.0469 8 6

3906.32 0.0619 0.0587 6 5

3906. 34 39.4272 0.0469 8 6

3906.48 0.1100 0.0757 8 5 3906.82 0.2036 0.0695 9 5 3907.40 0.1684 0.0894 7 2

3907.71 0.0839 0.0787 8 4

3908.23 / 0,1903 0. 0701 8 4

3908.32 0 ,1268 0.0633 8 2

3908.53 0.5993 0.0391 12 2 3908 . 57 0.2984 0.0736 8 3

3908.65 0 .0149 0. 0594 8 5

II J E" L BAND

9 8 0 8 2337.53 8 , 745630 NU3-«--«-* 5 6 3 4 648 .97 5, 110000 NU3*^

4 5 2 3 446 . 50 5,358633 NU3**

7 7 2 6 2 318.53 7,292008 NU3*-«-*

6 10 3 7 1538.23 0,369280 NU3

8 9 1 9 920.21 0,472318 NU3

9 10 1 10 1114,56 0,478334 NU3^

1 4 4 0 2129,65 4, 397010 NUl***

0 4 4 1 2129,63 4, 396748 NUl***

15 14 0 14 2073 ,66 14,00192 NUl

15 14 1 14 2073,66 14,00191 NUl

4 6 3 3 2282,59 5 , 330000 NU3^**

8 9 0 9 920,18 0,471417 NU3

2 5 3 3 504,00 11,35 NU 1 +

6 6 1 5 542 ,91 6,391209 NU3*-5^

1 5 3 2 508 ,81 64, 02 2NU2 +

4 7 0 7 586,26 0.239 NU1 +

1 6 0 6 446,71 0. 000172 NU3

2 5 2 3 446 , 50 0.039164 NU3

3 5 3 2 508,81 2. 720000 NU3-

6 6 2 5 552,92 5.960000 NU3-

7 7 2 6 709 . 60 7.292008 NU3*

4 8 6 3 3101,19 5 .032027 NU3***

4 7 5 3 1059.65 4. 903948 NU3-^

9 8 1 8 744 . 16 8. 745235 NU3*

9 8 0 8 744 . 09 8. 745630 NU3-W3 8 7 2 1590 . 74 3.5792 53 NU3*

1 4 1 4 224.83 0.017070 NU3

8 7 1 7 586.48 7. 746063 NU3

8 7 0 7 586.26 7. 747248 NU3

4 6 4 3 7 56.75 4.735129 NU3

4 6 3 3 661 . 56 7.34 NU1 +

0 5 3 3 504.00 4.25 2NU2 +

5 7 3 4 842 .38 6,30 NUl*

7 7 1 6 704. 22 7.336095 NU3*

4 5 2 3 446. 50 5. 358633 NU3

5 6 3 4 648 .97 5. 110000 NU3-

1 8 8 0 1789.10 1.901685 NU3

2 8 8 1 1789 . 10 1.901685 NU3

2 7 0 7 586.26 0.000274 NU3

3 6 4 2 757 .78 4,739627 NU3

6 6 1 5 542 .91 6,391209 NU3

3 7 6 2 1216.20 3,522863 NU3

1 5 4 2 610.12 4.264570 NUl*

2 7 6 1 1216.20 3 , 522866 NU3

3 8 2 6 982 .91 0,098024 NUl

4 9 2 7 1201 ,95 0, 180415 NUl

5 6 2 4 2211,21 6,352023 NU3***

4 7 4 3 2572,13 5,440000 NU3***

5 7 4 4 927 ,77 6 ,014663 NU3*

7 7 2 6 709 , 60 7,292008 NU3**

10 12 2 11 1774,74 0,875278 NU3

6 7 3 5 816,72 5,410000 NUB*

4 7 5 3 1059,65 4, 903948 NU3**

66
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

gm cm atm.

3908,73 0.0159 0,0852 8 4

3908,97 3.6252 0,0762 4 4

3909,22 0.3840 0,0446 9 1 3909,26 0.1280 0,0447 9 0

3909,36 0.0286 0,0637 6 5

3909,51 0.0445 0,0608 8 5

3909, 52 1.0211 0,0894 7 2

3909.86 0.0229 0,032 16 0

3910,03 0,1994 0,0381 12 3

3910. 16 0,6387 0,0885 7 3

3910.22 0,1823 0,0795 4 4

3910,58 1 ,6492 0,0728 9 5

3910,73 0,0135 0.0834 7 4

3910.86 0,0687 0.032 16 1 3911.21 0,0343 0,0598 6 5 3911 .27 0,0530 0,0388 10 1 3911.33 0,1589 0,0388 10 0

3911.45 0,0114 0,0587 6 5

3911.98 0,3936 0,0670 8 1 3912.30 0,0670 0.032 15 1 3912.32 0,0183 0,032 15 2

3912,34 0, 1607 0.0535 9 2

3912, 58 0.0425 0,0496 9 6

3912,69 8.8978 0,0397 10 1 3912,69 0.0142 0,0500 9 6

3912,98 2 .9643 0,0393 10 2

3913,15 0.5759 0.0952 4 2

3913,40 0.3505 0.0806 7 5

3913,56 0.0191 0,0607 9 5

3913,80 0.0312 0.0340 10 9

3913,80 0.0937 0.0340 10 9

3914,00 42.9027 0.0852 8 4

3914.12 0.2876 0.0774 7 4

3915.12 0.0142 0.0852 8 4

3915.35 0.0152 0.0928 6 2

3915.50 0,5083 0.0787 8 4

3915.65 0,0544 0.0559 9 1 3915.97 0,0353 0.0701 8 4

3916,06 0,9741 0.0535 9 2

3916,30 342 ,7574 0.0633 8 2

3916,35 92 ,7388 0.0598 6 5

3916,36 40,0471 0.0594 8 5

3916,44 0,0552 0.0736 8 3

3916,45 0,9627 0.0388 10 0

3916,59 30,9367 0.0587 6 5

3916.81 2.0463 0.0408 9 7

3916.81 6,1389 0.0407 9 7

3917. 19 120.1755 0.0608 8 5

3917.23 1037.6231 0.0446 9 1 3917.28 346.0373 0.0447 9 0

3917.73 0.1182 0.0885 7 3

3917.82 0.0408 0.037 14 3

3917.89 0.3299 0.0559 9 1 3918.78 0.0532 0.0774 7 4

.1" E" L BAND

1 3 4 o42 .90 6,30

i 4 2

9 '2 1 £^ 7 Q 9 1 9 . ly M II Q INU 9

Q p 1 00~J /i 1 A P0, 7 /j R 9 "3 R / '+9A99 Ml 1 9 -Ir -If- IN U 9

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Q 7 9

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X ^ X -5 9 i 1 9 9 /i A Q P A A f D , V C3 R qn Q A 1 0 , y\j Vol INMill U i 8 8 1 7 882,93 8,308658 NU3*

3 6 3 4 648 ,97 8.01 NUl*^^

67
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm~i

gm cm~2

cm"i

atm.

3919,06 0.0116 0.0626 7 4 3

3919,81 0.0306 0,0598 6 5 2

3920 , 06 1063 .9061 0,0670 8 1 7

3921,25 2 .5260 0.0844 9 4 6

3921.26 0 .1066 0.0952 4 2 2

3921,54 6 . 1053 0.0835 5 3 2

3921 ,63 0.0475 0.0774 7 4 3

3922,53 0,0577 0,0359 13 2 11

3922,82 0 .0429 0,0682 9 4 6

3922,90 0.1159 0.0607 9 5 5

3922,91 7.6227 0.0928 6 2 4

3922,99 0.0836 0.0674 9 3 7

3923,05 0.0940 0.0787 8 4 4

3923.08 0 .1723 0.0352 13 3 11

3923,45 143,8194 0.0774 7 4 3

3923 .72 95,1719 0.0701 8 4 5

3923.94 0,0805 0.0822 6 5 1 3924 .09 0.1802 0,0535 9 2 8

3924 . 3

1

149.1879 0.0736 8 3 6

3924. 35 0.2263 0.0879 7 3 4

3924.44 9.6121 0.0750 4 4 0

3924.47 0.0593 0.0388 10 1 10

3924 .50 0.1781 0.0388 10 0 10

3924.88 2.6192 0.0801 10 4 7

3925 .22 510. 5409 0.0894 7 2 5

3925 .31 319.3415 0.0885 7 3 4

3925.86 0.9200 0.0742 8 5 4

3925,99 0.2373 0.0373 10 8 3

3925,99 0.7121 0.0374 10 8 2

3925,99 0.0611 0.0559 9 1 8

3926 , 15 0.2360 0.0838 8 2 6

3926 ,52 0.0373 0.0879 7 3 4

3926,65 1.4309 0.0838 8 2 6

3926,90 0.5068 0.0674 9 3 7

3927.29 0.0228 0.0456 10 2 9

3927 , 37 0.2851 0.0731 11 4 8

3927,6 3 0.0289 0.0660 7 5 3

3928,01 2 1 .2671 0.0496 9 6 4

3928, 10 7,08 93 0.0500 9 6 3

3928 , 1

1

1,0370 0.0359 11 1 10

3928,25 3,1105 0.0358 11 2 10

3928,29 4,8510 0.0880 5 3 3

3928,74 0,2600 0.0682 9 4 6

3928.78 0,0869 0.0628 7 5 2

3929.09 0,0688 0.0467 10 1 9

3929.31 4,9355 0.0762 5 4 1 3929.37 287 ,9477 0.0952 4 2 2

3930.14 0,2678 0.0649 12 4 9

3930.40 0,0226 0.0431 6 6 1 3930,60 254, 1416 0,0787 8 4 4

3930,97 0,1379 0.0456 10 2 9

3931,09 0,1073 0,0737 5 4 2

3931.38 0.1602 0.0889 8 3 5

3932.00 4,6990 0.0801 8 6 3

J" Kc E" L BAND

8 0 8 744, 09 0. 000295 NU3

5 1 2251 ,86 4.266963 MUl*^?-*

7 1 6 704,22 7.336095 NU3

8 3 5 1050,15 3 . 141455 NU 1 3 0 3 136,77 0. 116055 NU3^^*

5 1 5 326 ,64 0.019115 NU3

6 3 4 2271 ,70 8,01 NU 1***

13 2 12 2042 . 38 0,881500 NU3

8 4 5 2764,71 7 , 216366 NU3***

8 5 4 1255.16 6,255627 NU3*

5 1 5 326 .64 0,254241 NUl

8 3 6 2630.21 7, 854581 NU3**^^

7 4 3 931 .22 5 . 440000 NU3**

13 1 12 2042.33 0.878880 NU3

6 3 4 648 ,97 8.01 NU1 +

7 4 4 927,77 6.014663 NU3

6 2 4 602,77 0.010677 NUl

8 2 7 885.62 8. 292239 NU3**

7 3 5 816.72 5.410000 NU3-

6 2 5 552.92 3.89 NUl*

2 3 300.35 0.008789 NU3

9 1 9 920.21 9. 744353 NU3**

9 0 9 920 .18 9, 744485 NU3**

9 3 6 1282 .92 3.465920 NUl

6 2 4 602 .77 6.352023 NU3

6 3 3 661.56 5.330000 NU3-

8 3 5 1050 . 15 0. 107233 NU3

9 8 2 2009 .87 3.624262 NU3

9 8 1 2009 .87 3, 624262 NU3

8 1 7 882.93 8, 308658 NU3**

7 2 5 2392 . 58 7,251910 NU3***

6 2 5 2161.30 3,89 NUl***

7 2 5 782 , 40 7.251910 NU3*

8 3 6 1006 . 12 7.854581 NU3*

9 2 8 2690 ,64 9.287364 NU3***

10 3 7 1538 .23 4. 032477 NUl

6 4 2 757.78 4. 143594 NUl*

8 6 3 1411 .65 5.032027 NU3

8 6 2 1411 .68 5.032058 NU3

1

1

1 11 1327. 14 0,483240 NU3

1

1

0 1

1

1327 . 14 0,483142 NU3

4 0 4 222 . 06 0.095779 NU 1 8 4 5 1122.72 7, 216366 NU3*

6 4 3 756 .75 4, 131192 NUl*

9 1 8 2688.10 9,293415 NU3***

5 2 4 416.22 0,024136 NU3

3 0 3 136 . 77 0, 116055 NU3

1

1

3 8 1813.26 4,836759 NUl

5 5 0 742 . 10 5,399718 NUl**

7 4 3 931.22 5 , 440000 NU3-

9 2 8 1080.38 9, 287364 NU3*

5 1 5 326 .64 0,003573 NUl

7 3 4 2462.87 6.630000 NU3***

7 3 4 842.38 7,42 2NU2 +

68
LINE HALF

FREQUENCY STRENGTH WIDTH J' K

cm ' cm ' cm~^

gm cm 2 U 1 1 1 -

3932 . 12 487 . 0765 0.0535 9 2 8

3932. 16 113.1350 0.0879 7 3 4

3932.53 160.4471 0.0388 10 1 10

3932 . 56 481.3514 0.0388 10 0 10

3934. 09 164.9429 0.0559 9 1 8

3934.65 0.2647 0.0838 8 2 6

3934.69 0.971

1

0.0889 8 3 5

3934.75 0.0184 0.0520 10 6 4

3934.85 0.0938 0. 0674 9 3 7

3935. 15 22 .0035 0.0885 3 3 0

3935.17 0.2344 0.0885 4 3 1 3935 .30 0.0917 0.0815 5 5 0

3935.77 61 .0285 0. 0431 6 6 1 3935 . 77 0 .0438 0.0340 14 2 12

3936. 54 0.0480 0.0682 9 4 6

3938 . 00 14, 4444 0 .0660 7 5 3

3938.06 1.0117 0.0430 10 7 4

3938 . 06 3 .0352 0. 0431 10 7 3

3938 . 34 57.9477 0.0607 9 5 5

3938.44 12 .4824 0.0755 6 4 2

3939.05 43 ,4443 0.0628 7 5 2

3940. 05 0.0771 0.0467 10 1 9

3940.07 0.0201 0.0431 6 6 1 3940 .27 0 ,0638 0.0815 9 4 5

3940 .29 3.8707 0, 0740 7 5 3

3940. 54 0. 1965 0.0760 9 2 7

3940.69 19.2321 0.0640 9 5 4

3941.27 0.0325 0.0760 9 2 7

3941 .64 0.0118 0.0608 8 4 4

3941 . 64 0.0162 0.0873 3 3 1 3941 . 93 0.0143 0.0628 7 5 2

3942. 34 0 .1797 0.0889 8 3 5

3942 .65 715.4263 0.0838 8 2 6

3942.81 253 .3967 0.0674 9 3 7

3943 .12 0.9857 0.0337 12 1 11

3943.17 0.3286 0.0337 12 2 11

3943. 57 0,0783 0,0793 8 4 4

3943.58 0.0668 0.0594 10 3 8

3944. 14 0,0434 0.0885 4 3 1 3944, 34 129 ,981

1

0.0682 9 4 6

3944,41 0,0157 0.0789 6 3 3

3944.47 0,0157 0. 0604 10 5 6

3945.19 0,0722 0.0818 8 3 5

3946.50 0,0858 0, 0392 1

1

8 3

3946. 50 0,2576 0,0391 1

1

8 4

3946.64 0,0772 0,0658 1

1

6 6

3947.15 68 .9486 0,0456 10 2 9

3947.25 0 .2907 0,0681 6 4 3

3947,47 201.6251 0, 0354 1

1

1 11

3947 . 48 67.2088 0,0354 1

1

0 1

1

3947 .76 0.0118' 0,0815 9 4 5 3947 .97 0.0145 0,0793 8 4 4

3948. 18 208.4119 0,0467 10 1 9

3948.69 0.0364 0,0760 9 2 7

II J Kc

c"E L Q AKin tJANL/

cm-1

8 2 7 885,62 8.292239 NU3

6 2 5 552,92 3.89 NU1 +

9 1 9 920.21 9.744353 NU3

9 0 9 920.18 9.744485 NU3

8 1 7 882 .93 8. 308658 NU3

7 2 5 782.40 7.251910 NU3**

7 3 4 842 .38 6.630000 NU3*

9 6 3 1631.41 6.440055 NU3*

8 3 6 1006.12 7.854581 NU3**

2 1 1 95.17 0.021579 NU3

3 1 2 173.36 0.056400 NU3i^

5 2 3 446.50 0.001850 NUl

5 5 0 742.10 5.399718 NUl

14 2 13 2327.90 0.895030 NU3

8 4 5 1122 .72 7.216366

6 4 2 757.78 4. 143594 NUl

9 7 3 1810.63 5. 133658 NU3

9 7 2 1810.63 5. 133660 NU3

8 5 4 1255.16 6.255627 NU3

6 2 5 552 .92 0.040211 NU3

6 4 3 756.75 4. 131192 NUl

9 1 8 1079.07 9.293415 NU3**

5 5 0 2406. 15 5.399718 NUl**

8 4 4 1131 .76 5. 540000 NU3*

7 3 4 842.38 0.052981 NU3

8 2 6 982 .91 8. 113471 NU3*

8 5 3 1255.92 6.258032 NU3

8 2 6 2595.81 8. 113471 NU3**

9 0 9 920. 18 0.000238 NU3

2 1 2 79.48 0.013176 NU3**

6 4 3 2398.39 4.131192 NUl**

7 3 4 842 .38 6.630000 NU3**

7 2 5 782.40 7.251910 NU3

8 3 6 1006,12 7.854581 NU3

12 1 12 1557,91 0.487287 NU3

12 0 12 1557,91 0.487254 NU3

7 3 5 816,72 5.02 NUl*

9 3 7 1216.27 8.878817 NU3*

3 1 2 173.36 0.056400 NU3**

8 4 5 1122.72 7, 216366 NU3

6 1 6 447.24 0.014823 NU3*

9 5 5 1474.99 7.532122 NU3*

8 0 8 744. 09 0.019318 NUl

10 8 2 2254.34 5.216541 NU3

10 8 3 2254.34 5.216540 NU3

1

1

4 7 , 1899.06 0.195288 NU3

9 2 8 1080.38 9.287364 NU3

6 1 6 447 .24 0.005871 NUl

10 1 10 1114.56 10.743553 NU3

10 0 10 1114.55 10.743597 NU3

8 4 4 1 131 .76 5. 540000 NU3**

7 3 5 816.72 5.02 NUl**

9 1 8 1079,07 9.293415 NU3

8 2 6 982.91 8. 113471 NU3**

69
LINE HALF

FREQUENCY STRENGTH WIDTH J' K Q ^ cm~i

gm cm-2 atm.

3948 .89 0.0105 0 . 0662 1

1

6 5

3949 .39 0,0379 0,0850 4 4 1 3949 .50 3.0760 0,0508 10 6 5 3950.00 48 5.5714 0,0889 8 3

3950, 13 9 .2298 0.0520 10 6 4

3950.59 43.7681 0.0873 3 3 1 395 1.39 0 .0041 0.0669 8 5 3

395 1.43 0.0119 0 . 0643 8 5 3

3951.61 0,0123 0. 0594 10 3 8

3951 • 62 0,0014 0.0612 10 5 5

3951.97 1,4100 0.0710 6 5 2

3952 . 08 0,0051 0.0781 10 6 5

3952 . 38 39 , 1454 0. 0793 8 4 4

3952.62 0,2199 0.0666 10 2 8

3952.77 0,0106 0.0480 7 6 1 3953 . 1

1

117,2356 0.0885 4 3 1 3953.55 2 .3121 0.0727 7 4 3

395 3.72 0.0363 0 .0666 10 2 8

3953.74 0.0232 0 .0864 9 3 6

3954. 55 0.0015 0.0665 6 5 1 3955 . 17 0.0387 0.0885 A- 3 1 3955.25 31.8921 0.0815 9 4 5

3955 . 54 0 .0070 0.0850 4 4 1 3955 . 91 0.0063 0 .0648 10 4 7

3956.14 0.0028 0.0588 1

1

5 7

3956.52 0.0022 0. 0643 8 5 3

3956 .59 0.1401 0.0864 9 3 6

3956.85 98.2710 0 . 0760 9 2 7

3957.28 0.0086 0.0671 10 5 5 3957.43 0,0962 0.0327 1

3

1 12

3957 . 45 0,2887 0.0327 13 2 12

3957.85 0,0225 0 . 0 804 6 3 4

3958 . 04 0,1054 0.0928 5 2 3

3958 . 12 9,5916 0. 0483 7 6 2

3958 . 15 28,7734 0.0480 7 6 1 3958.21 42 ,0275 0. 0706 8 5 4

3958.30 0,0471 0.0337 9 9 0

3958.66 3,6727 0.0630 8 6 2

3958 .90 0.0068 0.0725 10 6 4

3958.95 0.9790 0 . 0425 11 7 5 3959.05 0.3264 0 . 0446 1

1

7 4

3959.22 0.0054 0.0692 8 4 4

3959 .27 0. 1106 0.0725 13 5 8

3959.65 33 ,4287 0.0594 10 3 8

3959 . 9

1

2 ,8344 0.0666 5 5 1 3959. 93 7,8365 0.0604 10 5 6

3960.81 7 , 8490 0. 0789 6 3 3

3960.88 0 ,0407 0 . 0666 10 2 8

396 1 . 62 5,9272 0 .0643 8 5 3

3961.69 18,9596 0.0850 4 1 3961.73 78,9862 0.0397 1

1

2 10

3962 .05 25 ,4178 0.0335 1

2

1 12

3962.05 76,2535 0.0335 12 0 12

3962.21 26.5075 0.0402 11 1 10

J" K a '^c E" L BAND

cm"i

11 3 8 1813.26 0,189337 NUl

3 1 2 173.36 0.097 NUl^t

9 6 4 1631 .27 6.439836 NU3

7 3 4 842 .38 6.630000 NU3-

9 6 3 1631.41 6.440055 NU3

2 1 2 79.48 0.013176 NU3

8 3 6 1006.12 0.064192 NU3*

7 4 4 927.77 3.953657 NUl*

9 3 7 1216.27 8.878817 NU3**

9 2 8 1080.38 0.021627 2NU2

6 3 3 661.56 0.023375 NU3

9 3 6 1282.92 0.071662 2NU2

7 3 5 816.72 15.02 NU1 +

9 2 7 1201.95 9.000870 NU3*

6 5 2 888.60 5.265222 NUl*-^

3 1 2 173.36 0.056400 NU3-

7 2 6 709.60 0.048724 NU3

9 2 7 2818.40 9. 000870 NU3*^^*

8 3 5 2670.79 8.066869 NU3^*-**

6 3 4 648 .97 0.021403 NU3**

3 1 2 1772.41 0.056400 NU3^^**

8 4 4 1131.76 5. 540000 NU3-

3 1 2 173 .36 0.097 NUl**

9 4 6 1340.89 8.354292 NU3**

10 5 6 3383,36 8,747542 NU3***

7 4 4 927,77 3,953657 NUl^-«-

8 3 5 1050.15 8.066869 NU3*

8 2 6 982.91 8. 113471 NU3

9 5 4 1477.31 7. 545052 NU3**

13 1 13 1806.78 0.4861 10 NU3

13 0 13 1806.78 0.486060 NU3

5 0 5 325.35 0.123125 NUl*

4 0 4 222.06 0.096503 NU3*

6 5 1 888.63 5.265494 NUl

6 5 2 888.60 5.265222 NUl

7 4 3 931.22 9.52 NU1 +

8 8 1 1789.10 8.403719 2NU2

7 3 5 816.72 15.00 2NU2 + 10 3 7 1538.23 0.095771 NUl

10 7 4 2054.40 6.588139 NU3

10 7 3 2054.40 6.588161 NU3

8 2 7 885.62 0.045112 NU3*

12 5 7 2300.80 11.223190 NU3

9 3 7 1216.27 8.878817 NU3

5 3 2 508.81 0.007283 NU3

9 5 5 1474.99 7.532122 NU3

6 1 6 447.24 0.014823 NU3

9 2 7 1201.95 9.000870 NU3**

7 4 4 927.77 3.953657 NUl

3 1 2 173.36 0.097 NU1 + 10 2 9 1293,66 10.281117 NU3

11 1 11 1327,14 11,742858 NU3

11 0 11 1327, 14 11.742873 NU3

10 1 9 1293,04 10.283342 NU3

70
LINE HALF

FREQUENCY STRENGTH WIDTH J' K cm ~' ^rn*~l

/^ T-r\ fT\ ~ 2 yrn crii atm.

3962.70 0.0042 0.0804 6 3 4

3963.35 0.0467 0.0775 10 5 6

3963. 49 0,0032 0.0483 7 6 2

3963.51 0.0095 0.0480 7 6 1 3963.69 0.0321 0.0378 7 7 0

3963.78 16.9862 0.0648 10 4 7

3964.08 0.0020 0.0643 8 5 3

3964,26 0.0588 0.0667 10 6 5 3964,37 0.0259 0.0864 9 3 6

3964.61 4.1382 0.0665 6 5 1 3964.72 0.9442 0.0648 5 5 0

3964.81 23.2044 0.0671 10 5 5 3965.09 0,0427 0.0886 4 3 2

3965.58 0,0222 0.0698 5 5 1 3965.66 0,0189 0.0750 9 5 5

3965.86 0,0174 0.0928 5 2 3

3965.97 0,0195 0.0928 5 2 3

3966. 19 1 .1648 0.0675 7 5 2

3967. 55 11.2730 0.0804 6 3 4

3968.88 0.0240 0.0528 8 6 3

3969. 14 109.9538 0.0666 10 2 8

3970.00 0.0365 0.0859 5 4 2

3970.70 3 .0892 0.0515 11 6 6

3970.92 2.0857 0.0669 8 5 3

3971.09 0,0035 0.0750 9 5 5

3971.36 0.0182 0.0858 7 2 5 3971 .49 0.0242 0.0320 14 2 13

3971.49 0.0729 0.0320 14 1 13

3972. 15 70.0220 0.0864 9 3 6

3972.22 1.0302 0.0536 11 6 5

3972.66 37.8942 0.0898 5 3 2

3973.44 0,0304 0.0779 9 6 3

3973.78 0,1300 0.0649 6 5 2

3973.90 52,6906 0.0928 5 2 3

3974.70 23.3262 0.0775 10 5 6

3974.76 0.1479 0.0817 10 3 7

3974.89 5.3573 0.0378 7 7 1 3974.89 16.0718 0.0378 7 7 0

3975.11 35.3837 0.0515 11 3 9

3975.73 0.0126 0.0898 5 3 2

3975.95 9.1607 0.0360 12 2 11

3976.08 0.0239 0.0654 9 5 4

3976. 16 27.4855 0.0361 12 1 11

3976.20 2 .6796 0.0692 8 4 4

3976.33 8.4533 0.0325 13 0 13

3976.33 25.3539 0.0325 13 1 13

3976. 53 9.4335 0.0750 9 5 5

3976.97 0.0037 0.0804 6 3 4

3977.47 0.0590 0.0630 7 4 4

3978.56 0.0031 0.0750 9 5 5

3978.84 9.1041 0 .0858 7 2 5

3979.38 0.3697 0.0665 9 6 4

3979.66 0,1322 0.0429 12 7 6

3979.67 12,0178 0.0528 8 6 3

ill J K a '^c E L BAND

5 0 5 325.35 0.123125 NUl**

9 4 5 1360.28 2.80 NUl*

6 5 1 2552.87 5.265494 NUl***

6 5 2 2552.85 5.265222 NUl***

6 6 1 1045.07 6.401516 NUl*

9 4 6 1340.89 8.354292 NU3

7 4 4 2569.52 3.953657 NUl***

10 4 6 1616.51 0. 114652 NU3

8 3 5 1050.15 8.066869 NU3**

6 3 4 648.97 0'.021403 NU3

5 3 3 504.00 0.007097 NU3

9 5 4 1477.31 7. 545052 NU3

3 1 3 142.28 0.026225 NU3*

5 2 4 416.22 0.001149 NUl

8 4 4 1131 .76 7.37 NUl*

4 0 4 1817.50 0.096503 NU3«-**

4 0 4 222 .06 0.096503 NU3**

7 3 5 816.72 0.041795 NU3

5 0 5 325.35 0.123125 NUl

7 5 2 1059.85 5. 144364 NUl*

9 2 7 1201.95 9.000870 NU3

4 1 3 275.52 0.465 NUl*

10 6 5 1875.00 7.773013 NU3

8 3 6 1006 .12 0.064192 NU3

8 4 4 1131.76 7.37 NUl**

6 1 6 447.24 0.182385 NUl*

14 0 14 2073.66 0.488990 NU3

14 1 14 2073.66 0.489010 NU3

8 3 5 1050. 15 8.066869 NU3

10 6 4 1875,53 7,774282 NU3

4 1 3 275.52 0.089700 NU3

9 3 6 1282 .92 0.039684 NUl

6 2 5 552.92 0.004423 NUl

4 0 4 222.06 0.096503 NU3

9 4 5 1360.28 42.8 NU1 +

9 3 6 1282 .92 9.029655 NU3*

6 6 0 1045.07 6.401518 NUl

6 6 1 1045.07 6.401516 NUl

10 3 8 1446. 16 9.881611 NU3

4 1 3 1875.49 0.089700 NU3***

11 2 10 1525.13 11.275004 NU3

8 4 5 1122.72 6.99 NUl*

11 1 10 1524.87 11.275820 NU3

8 2 7 885.62 0.045112 NU3

12 0 12 1557.91 12.744460 NU3

12 1 12, 1557.91 12.744430 NU3

8 4 4 1131 .76 17.37 NU1 +

5 0 5 1920.76 0.123125 NUl***

7 1 7 586.48 0.007119 NUl

8 4 4 2771 .71 17.37 NUl***

6 1 6 447.24 0.182385 NUl

9 4 5 1360.28 0.066893 NU3

1 1 7 5 2321.89 7.967474 NU3

7 5 2 1059.85 5, 144364 NUl

71
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ' gm cm 2

*~ I LI Motm.

3979.68 3 .0846 0,0852 8 3

3979.74 8.2754 0,0588 11 5 3979.91 0.3967 0,0453 12 7

3979.92 4.0049 0.0502 8 6

3980.34 0.3065 0, 0645 9 5 3980.43 0.0112 0.0838 4 4

3980.82 12 .3671 0.0563 11 2 3981.06 0.0044 0.0654 9 5

3981 . 36 0 .0018 0.0378 7 7

3981 . 36 0.0053 0.0378 7 7

3982. 14 17.3995 0.0603 11 4

3982.21 18 .2742 0.0859 5 4

3982.73 0.0273 0.0817 10 3

3982.89 21 .3901 0.0886 4 3

3983.09 0.0682 0.0846 6 4

3983.35 0.0018 0,0798 9 4

3983.47 0.0709 0.0679 13 6

3984. 1

1

0,0063 0.0850 4 4

3984,46 0.0055 0.0590 9 6

3984.58 0.0195 0.0451 13 3

3984.64 0 .0260 0.0785 6 6

3984.70 0 .00 16 0.0739 7 3

3985 . 02 1 ,2442 0.0778 1

1

5

3985 . 16 0,0040 0.0528 8 6

3985 . 33 0,0013 0.0502 8 6

3985.37 0 ,0082 0.0320 15 1 3985.37 0 ,0244 0.0320 15 2

3985.62 0,0045 0.0410 8 7

3985.62 0,0135 0.0410 8 7

3986.05 11,9396 0.0654 9 5 3986. 18 0,0436 0.0600 7 5 3986.20 0,0020 0.0798 9 4

3986.47 0,0021 0.0838 4 4

3986 . 78 0,0070 0.0886 4 3

3986.84 0,0039 0.0654 9 5 3988.67 0,1418 0.0754 12 5 3989.06 0,0126 0.0846 6 4

3989.42 0,0116 0.0803 8 6

3989.49 24,5023 0. 0346 13 2 3989.60 3,7992 0.0447 12 3

3989.61 8,1702 0.0338 13 1 3989.85 2,6353 0. 0700 11 5

3990.23 5,5069 0.0798 9 4

3990. 30 2 ,7420 0.0320 14 1 3990. 30 8,2322 0.0320 14 0

3990.43 0,0088 0.0536 9 6

3990.61 0,2154 0. 0646 8 6

3990.70 73,9364 0.0817 10 3

3991 . 12 0,3012 0.0516 12 6

3991 . 23 0,0025 0.0410 8 7

3991.41 0,2760 0.0889 6 3

3992.30 0,0077 0.0775 10 5

3992. 52 5 ,6070 0.0838 4 4

3992.57 11,4273 0.0475 12 2

J" u Kc E" L BAND

cm"i

c; 7 AD

7 n Q AO n A R R 1 Q 9 Mill InU X 7 J. \-/ A 1X 71 1X Rij # 77( ( 8 . 747 Ml 1 3

5 1

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7 4 2 32 1 ,94 7 . 967606 NU3

2 7 3 1059.65 5, 142711 NIJ

1

A g7 7 X1 A7 1X A0 .• (1. 0 7( MI I 3 n 1X 3 1 A p ^ 9 ft n . n 7 3 1 Kit J 1 ^

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R 1 n A. 7 1 S ft 1 - "^4 X (J X • -J " 9-7« 43ftQ45 '-rU(J7'-r-7 Nn3

2 4 X 3 275.52 n . 4A 5 NU 1 +

7 9 Au 1 282.92 9.0 7 9 A 5 5 Ml 1 3-**'-Jt 2 3 X _^ 1X 4 A7 .

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Au ^ U ^ \J • ^ X 1 -7 9744ft NIJ 1 8 1 2 5 7 2300.80 4 , 44 317 NU 1

1 3 1X 2 1772.41 X f ( t. • ^ X 0.097 NU 1 -X-Tt-^t 3 8 3 A 1006.12 X W W 'w' • ±. c~ 0.01 9449 2NU2

1J- 0\J 1 3 3 X X 2 248.16 1.17 8730 NU3

1 1X 4 399 . 46 ? . 8 5 7 A ' » A

A 7f 1X 7 S ft A 4ft nU»UU7AaU 000770 M I J 3 -J?" IN _3 ^ 71 7 X D X D • X 7 5-73 NU 1 +

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1 4 1 5 n 1 5 ? 3 5ft .44 0.491 500 NU3

1 7 A 2 1216.20 6.263414 NU 1*

2 7 A 1216.20 X £- X U • c - W 6 . 263444 NUl*

A « A. 1X X1 ?A ?A .. 7I A2 Au .• 997 7 NU 1 +

3 7 TA A\J 709 - fiO 0.00 97 05 NU 1 R -1

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1 1 X X 3 Qy 1 695 . n3 1 n. 873594 NU3

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A X U 1 724.72 8 . 79 8 8 m NU3

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72
LINE HALF

FREQUENCY STRENGTH WIDTH J cnn~i

gm cm -2 otm.

3993.32 0.0575 0.0757 4 4

3994. 93 0.9051 0.0552 12 6

3995.03 34.1141 0. 0846 6 4

3995.03 23.8564 0,0824 10 4

3995.96 0,3032 0,0620 10 5 3996. 14 0.0048 0,0785 6 6

3996.35 0.0138 0,0700 13 5

3996.84 2.2435 0,0410 8 7

3996.84 6.7304 0,0410 8 7

3996.92 0.8258 0. 0564 12 5 3997.83 0.8406 0,0610 7 6

3998.02 0,0538 0.0770 9 3

3998.81 1 .7479 0.0548 12 4

3998.89 0.1225 0.0590 9 6

3999.31 0,0185 0.0757 4 4

3999.72 0,0112 0.0726 11 4

3999.82 0,6517 0.0592 8 6

4000. 00 0.0510 0.0889 6 3

4000.20 0.1610 0.0578 10 6

4000. 32 1 .4678 0.0558 9 6

4000. 39 0.8194 0.0739 7 3

4000.48 0.0018 0.0751 5 4

4000.75 0.0021 0.0587 12 7

4001 .20 4.4214 0.0536 9 6

4001 .28 0,2822 0.0578 7 6

4001 .40 0,0455 0.0889 6 3

4001 .62 0,0013 0. 0661 10 5

4001.69 0 ,0044 0.0709 7 3

4001.82 0 ,0060 0.0859 5 4

4001 . 84 0,0824 0.0866 5 3

4002.06 0.2160 0. 0568 6 6

4002.47 0.0022 0.0351 8 8

4002.47 0,0066 0.0351 8 8

4002.70 0,1506 0.0770 4 4

4002.71 0,0022 0,0658 12 3

4002.77 0,8874 0,0330 14 2

4002 . 82 2,6561 0.0330 14 1 4002 .86 0,7343 0.0320 15 0

4002.86 2,2163 0.0320 15 1 4002.86 2,8563 0. 0394 13 3

4002 . 98 0.0106 0.0757 4 4

4003.09 0.6496 0.0552 6 6

4003.81 0.0868 0.0553 8 5 4004. 37 0.0294 0.0792 7 6

4004.69 1 . 1902 0.0411 13 2

4004.73 0.0187 0.0561 11 6

4005.43 7 .6069 0.0752 11 3

4006.63 0.2524 0.0658 9 4

4006.97 0.0017 0.0444 9 7

4007.00 0.0050 0.0443 9 7

4007. 37 0.0015 0.0536 9 6

4007.64 12 .9864 0.0785 6 6

4008.59 137.9963 0.0889 6 3

4009. 56 0.0031 0.0788 7 4

707-944 O - 64 - 6

J" Ka Kc E" L BAND

cm-1

0 3 9<c 1 212.15 n . ni 654? NU 3*

6 1

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6 5 2144.12 9 , 054429 NU3

3 5 1 4 399 .46 0,536 NU1 +

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5 1 0 3 8 1 446 .16 0.084234 NU3

1 5 4 399.46 2.857 2NU2**

9 1 2 4 8 2205.65 4,43448 NU 1

1 7 6 2 1216 . 20 6.263414 NU 1 2 7 6 1 1216.20 6 .263444 NUl

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2 7 4 3 931.22 0. 017690 NU3

6 9 0 9 920.18 0.01 1425 NUl

9 1

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3 9 4 6 1340.89 0.059724 NU3

1 3 2 2 206.30 0.015552 NU3-^

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2 8 4 5 1122.72 0. 035676 NU3

3 5 1 4 399,46 0,202769 NU3**

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4 8 5 3 1255 .92 5,013867 NUl

4 7 1 7 586 . 48 0,009220 NU3

2 5 0 5 325.35 0,000921 NU3*

6 1 2 5 7 2 300.80 0 , 124645 NU3

3 8 5 4 1255.16 5 , 006530 NUl

1 7 4 4 927.77 0 ,017491 NU3

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5 6 0 446 . 7

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1 6 4 2 757 .78 0.005721 NU3

0 7 7 1 1394,86 7. 402783 NU

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1 4 0 4 222 . 06 0 . 000274 NU3

9 1 1 3 8 3441 . 09 10.744435 NU3**

13 1 3 2 1 2 2042 .38 13.271150 NU3

13 1 3 1 12 2042 .33 13.271580 NU3

1 5 1

4

0 14 2073.66 14.743490 NU3

1 5 1

4

1 1

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2073 . 66 14, 743490 NU3

1

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1 2 3 1 0 1962 .55 11. 407070 NU3

0 3 2 1 212.15 0.016542 NU3**

0 6 4 3 756.75 0.00 5 704 NU3

4 8 2 7 8 8 5.62 0.015469 NUl

I 7 3 4 842 .38 0-0042 14 NU 1

1 1 1 2 2 1 0 1960 .22 11.888730 NU3

5 1

1

4 8 1843 , 02 0.111521 NU3

8 10 3 7 1538 ,23 9.899853 NU3

5 9 2 8 1080 , 38 0.033499 NU3

3 8 6 2 1411 ,68 6. 142105 NUl*

2 8 5 3 1411,65 6. 141896 NUl*

3 8 5 4 2919,63 5.006530 NU 1**

1X J. 4 399 .46 ? - 8 5 7 2NU7 +

3 5 1 4 399 ,46 0,202769 NU3

4 6 1 5 542 ,91 0. 147419 NUl*

73
LINE HALF

FREQUENCY STRENGTH WIDTH J' cm ~^ cm ~^ cm~^

gm cm~2 atm.

4009,81 0.1384 0.0875 6 2 4010.29 0.0295 0.0795 5 4

4010.66 0.0152 0. 0866 5 3

4010.78 0.5121 0.0503 13 6

4011.05 0.6318 0.0661 10 5 4011 . 17 2 .1902 0.0709 7 3

4012.22 0.0819 0.0588 8 4

4012.64 28.7486 0.0757 4 4

4014.00 1 .0931 0.0351 8 8

4014. 00 3.2793 0.0351 8 8

4014.00 1.1512 0. 0488 13 4

4014.07 0.0126 0.0539 12 6

4014.33 0.0205 0.0562 11 7

4014.39 2.5230 0.0721 12 5 4015.29 5 .0402 0.0810 11 4

4015.73 0.2142 0.0360 14 3

4015.91 0.7129 0.0330 15 2

4015 . 93 0.2377 0.0320 15 1 4016.31 0 .00^8 0.0755 6 6

4016.66 0.2622 0.0320 16 1 4016.66 0.7867 0.0320 16 0

4016.69 0.6430 0.0370 14 2

4016.90 0.5487 0.0531 13 5 4016.93 6.4797 0.0658 12 3

4017.60 0.0256 0.0875 6 2

4018.02 0.0011 0.0351 8 8

4018.04 0.1735 0.0573 13 6

4018.22 0.8306 0. 0444 9 7

4018.25 2 .4918 0.0443 9 7

4018.46 9.2903 0.0757 4 4

4018.59 0.0228 0.0875 6 2

4018.83 0.0010 0.0543 10 6

4019.49 41 , 1748 0.0866 5 3

4019. 54 0.0255 0.0595 11 5 4019.68 1 .4213 0.0586 10 6

4020.01 0.0054 0.0795 5 4

4020. 03 0.9109 0.0751 5 4

4021.04 1 .5364 0.0788 7 4

4021.48 0.0014 0.0594 5 5 4021 . 56 0.0113 0.0846 6 4

4022.14 0.4791 0.0540 10 6

4022.65 0.0094 0.0757 4 4

4022.94 0 .0024 0.0371 9 8

4023.97 0.0156 0.0563 10 7

4024. 90 0 .0136 0. 0866 5 3

4025.39 69.1862 0.0875 6 2

4025.39 0 .0940 0.0824 6 4

4025.96 0 .0788 0.0779 5 4

4026.41 0.0054 0.0502 12 7

4026.84 0.7200 0.0566 13 3

4027. 53 0 .0479 0.0869 7 3

4027.62 0.0065 0.0515 11 7

4027.91 0.0140 0.0522 9 5 4027.95 0.0017 0. 0465 10 7

Kc

I" J Ka Kc E L BAND

cm~i

4 5 0 5 325.35 0.069891 NU3-"-

1 4 2 2 315 .79 0.042579 NU3^;-

3 4 1 4 224.83 0.025200 NU3-^-

8 12 6 7 2433.85 10.260880 NU3

5 9 4 6 1340.89 3.272354 NUl

5 6 0 6 446.71 0.130226 NUl

5 8 1 8 744. 16 0.007182 NUl

0 3 2 1 212 .15 0.016542 NU3

0 7 7 1 1394.86 7.402783 NUl

1 7 7 0 1394.86 7,402783 NUl

10 12 4 9 2124.98 11.473010 NU3

6 12 4 9 2124.98 0, 124675 NU3

5 11 5 6 1999.02 0.081625 NU3

7 1

1

5 6 1999.02 10.047055 NU3

7 10 4 6 1616.51 9.709460 NU3

12 13 3 11 2248 . 16 12.856270 NU3

14 14 2 13 2327.90 14.267060 NU3

14 14 1 13 2327.88 14.267240 NU3

0 6 3 3 661 . 56 0.000843 NUl

16 15 1 15 2358 .44 15.743100 NU3

16 15 0 15 2358.44 15.743100 NU3

12 13 2 11 2246.98 12.866510 NU3

9 12 5 8 2275.44 10.979590 NU3

9 11 3 8 1813.26 10. 744435 NU3

4 5 0 5 325.35 0.069891 NU3^*

1 7 7 0 3109.98 7.402783 NUl^*

7 12 6 6 2437. 56 10.408370 NU3

3 8 6 2 1411.68 6. 142105 NUl

2 8 6 3 1411.65 6.141896 NUl

1 3 2 2 206.30 0.015552 NU3

4 5 0 5 1920.76 0.069891 NU3^«-^

4 9 3 7 1216.27 0. 029596 2NU2

3 4 1 4 224.83 0.025200 NU3-

6 11 3 9 1695.03 0.072485 NU3

5 9 5 4 1477.31 4.857731 NUl

1 4 2 2 315.79 0.042579 NU3*-«-

2 5 0 5 325.35 0.000921 NU3

4 6 1 5 542.91 0. 147419 NUl

1 6 1 6 447.24 0.000003 NU3

3 5 1 4 2000.90 0.536 NUl^*-*^

4 9 5 5 1474.99 4. 830967 NUl

0 3 2 1 1819.34 0.016542 NU3**

1 8 7 2 1590.74 7.261215 NUl^^

4 10 5 5 1724.72 0.051622 NU3

3 4 1 4 1821.61 0.025200 NU3-it*

4 5 0 5 325.35 0.069891 NU3

2 5 2 3 446.50 0.086601 NU3-55- 2 4 2 3 300.35 0.034972 NU3--

5 12 5 8 2275.44 0. 108157 NU3

10 12 3 9 2105.90 11.684530 NU3

4 6 1 5 542 .91 0. 214427 NU3-X4 11 5 7 1985 .83 0. 077402 NU3

5 9 2 8 1080.38 0.019752 NUl

4 9 6 3 1631.41 6. 01 9433 NUl^

74
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kc

cm "*1 nm rm ~ ^ U 1 1 1 W 1 I I atm.

4028 .08 0.2084 0,0430 14 1

1

4028 . 16 0 .0031 0.0757 4 4 1 4028,81 0.0024 0. 0764 8 2 6

4028.90 0.0142 0,0645 6 6 1 4029. 14 0.0010 0.0797 9 3 6

4029.38 0.0015 0.0523 13 6 7

4029.74 14.7533 0.0795 5 4 1 4029.92 0.0486 0.0519 10 7 3

4030.03 0.0089 0.0619 7 6 2

4030.24 0.0933 0,0538 9 7 3

4031.39 14.8720 0,0812 5 4 1 4032. 56 0.0314 0,0516 9 7 2

4032. 58 2 .7892 0,0797 9 3 6

4033. 17 0 .0013 0.0681 8

-2 5

4033.40 0.0267 0.0583 8 6 3

4033.55 0.0079 0.0869 7 3 4

4033,68 0.4733 0.0786 10 4 6

4034. 08 0.0456 0.0509 8 7 2

4034, 50 1.2038 0.0371 9 8 1 4034,50 4.3475 0.0772 12 4 8

4034, 84 0.1375 0.0498 8 7 1 4035 . 10 0.4013 0.0371 9 8 2

4035. 12 0.0174 0.0824 6 4 2

4035,44 0.0015 0.0759 11 7 4

4035,49 0.0146 0.0779 5 4 2

4035.74 0.0089 0.0869 7 3 4

4036.31 0. 1196 0. 0479 7 7 1 4036 , 43 1.2115 0 .0764 8 2 6

4036. 51 0.0399 0.0476 7 7 0

4036,68 0.1327 0. 0618 11 6 6

4036.96 O.OOlO 0.0337 9 9 0

4038.51 0.0020 0.0533 7 5 3

4039.26 0.8278 0.0465 10 7 4

4039.40 0.2759 0.0460 10 7 3

4039.97 0.0060 0.0540 9 6 4

4040.05 0.4780 0.0676 11 5 6

4040. 19 0.0048 0.0795 5 4 1 4041 . 13 0.0263 0.0840 7 4 3

4041 .27 0.0132 0.0692 8 4 5

4041.32 0.0158 0.0496 10 5 6

4043. 10 0.0199 0.0804 6 3 4

4043.38 0.4133 0.0523 11 6 5

4043,38 0.2882 0.0703 6 4 3

4043.96 23 .9504 0.0869 7 3 4

4044.8 6 47 .0066 0,0824 6 4 2

4045.03 39 .4195 0,0779 5 4 2

4046.71 0.0024 0.0692 8 4 5

4048.22 0.6493 0.0681 8 3 5

4048 .43 0.0064 0. 0614 8 3 6

4048.81 0.1731 0.0337 9 9 1 4048,81 0,5193 0.0337 9 9 0

4050 . 34 0.1060 0.0655 12 6 7

4050,35 0,3876 0.0719 13 4 9

4050.75 0,0048 0.0840 7 4 3

J" Q Kc E" L BAND

1 3 4 1 0 2426.22 12.476350 NU3

3 2 2 1 0 1 3 . 8 1 0.015552 Kit 1 -if. J' Jt.

1 N U 3 * ^ *

1 i 1 P A /( P A 1 /i '2 Q D A

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1 1 1 5 86.48 0,143980 M 1 1 1 NU i

—J1 5 3 10 59.65 0 . 004 / 34 M 1 1 O NU 3

1 U 5

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1 7 1 Q 7 7 /. P O A A /i 4. 5cS aU64 MNU1 1 1i D u o Ml 1 ^ IN U J; D i J A . y i A 0 1 /i /. 0 7 U . A i M-M- A r INU M 1 1 ^J

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Q0 i1 7 P A 1 A i ' o y . 10 p /i A 'a 7 1 o o . H-0 illy NU 1

1 1 5 6 19 99.02 1 /. c o c o o 4.458582 NU 1 12 4 8 2205.65 11.537610 NU3

6 2 4 602.77 0.157817 NU3*^<-

75
LINE HALF

FREQUENCY STRENGTH WIDTH J' Ka

» cm"' cm 1 gm cm -2

cm 1 aim.

4050.8b 0,0090 0.0496 10 6 5

4050.86 0,0135 0.0572 12 5 7

4051. 19 0,0103 0.0544 9 4 6

4051 .64 0,0012 0.0482 12 8 5

4051,71 0 ,0014 0.0798 5 5 1 4051 . 84 0,0037 0.0804 6 3 4

4052.16 6,6138 0.0692 8 4 5

4053.09 0,0012 0.0614 8 3 6

4054.41 0 ,0044 0.0707 10 3 7

4054. 97 0,1359 0.0396 10 8 2

4054.97 0,4078 0.0396 10 8 3

4054. 98 0,0236 0.0774 6 4 3

4055.03 0,0130 0.0779 5 4 2

4055.35 0.0033 0,0459 12 8 4

4055.36 0.0156 0.0824 6 4 2

4055.75 0.0049 0.0812 5 4 1 4056.45 0.0040 0,0719 5 5 0

4056.72 0,0044 0.0471 1

1

8 4

4057.76 3 ,1892 0.0614 8 3 6

4058. 15 0,0015 0.0459 11 8 3

4058.95 0,0747 0.0475 11 7 5

4059. 50 0,2241 0.0468 11 7 4

4060. 38 13,1213 0.0840 7 4 3

4060. 58 9 ,9877 0.08C4 6 3 4

4060.77 0,0505 0.0841 8 4 4

4060.86 0,0103 0,0448 10 8 2

4061.65 0,1702 0,0622 10 4 6

4062.75 0,0182 0.0437 9 8 2

4062.89 0 .0061 0.0434 9 8 1 4063.73 0,0049 0.0774 6 4 2

4064.07 0,0059 0,0417 8 8 1 4064. 10 0 ,0176 0.0416 8 8 0

4064.42 0 .0044 0,0774 6 4 3

4064.46 0.0078 0.0645 5 5 0

4065.42 0,0335 0.0530 12 6 6

4065.84 0,0188 0. 0794 7 2 5 4065.86 0,0234 0.0640 5 5 1 4066. 01 0,7051 0.0798 5 5 1 4066.37 0,0012 0.0462 11 6 6

4067.35 0 ,0033 0.0804 6 3 4

4067.75 0,0014 0. 0795 4 4 0

4068.25 0 ,0022 0.0692 8 4 5

4069.26 0,0865 0.0694 5 5 1 4069.62 0,0036 0.0739 9 7 2

4069.84 0 .0011 0.0614 8 3 6

4069. 96 0,0044 0 .0840 7 4 3

4070.09 0.0093 0.0841 8 4 4

4070, 16 0,2192 0.0627 8 6 3

4070.61 0.0526 0.0350 10 9 1 4070,61 0,1579 0,0350 10 9 2

4070,62 0 ,0852 0.0694 6 5 2

4070,98 0,0339 0. 0690 12 5 7

4072,50 0.0465 0.0804 8 3 5 4072,70 0.5343 0.0646 7 4 4

J" Kc E" L BAND

cm-1

10 3 8 1446 . 16 0.026178 NUl

12 3 10 1962.55 0,053237 NU3

9 1 9 920.21 0,006488 NUl

12 6 6 2437.56 0.066727 NU3

4 2 2 315.79 0.0215 NUl*

5 1 5 326.64 0.030200 NU3**

7 1 6 704.22 0.47 NU1 +

7 0 7 586.26 0.125531 NUl**

10 0 10 1114.55 0.007326 NUl

9 7 3 1810.63 7.138077 NUl

9 7 2 1810.63 7. 138103 NUl

5 2 4 416.22 0.055572 NU3*

4 2 3 1907.99 0.034972 NU3***

12 6 7 2433.85 0.066188 NU3

5 2 3 2053.98 0.086601 NU3***

4 1 4 1821.61 0.0967 NUl***

5 0 5 325.35 0.000043 NUl

1

1

6 5 2144. 12 0.043132 NU3

7 0 7 586. 26 0.125531 NUl

11 6 6 2142.69 0.043025 NU3

10 6 4 1875.53 5.881509 NUl

10 6 5 1875.00 5,877228 NUl

6 2 4 602 .77 0,157817 NU3

5 1 5 326.64 0,030200 NU3-

7 2 5 782.40 0,247061 NU3*

10 6 5 1875.00 0,025193 NU3

10 2 9 1293.66 0,021601 NU3

9 6 3 1631 .41 0.012333 NU3

9 6 4 1631.27 0.012330 NU3

5 1 5 326.64 0.0787 NUl*

8 6 2 1411.68 0.004043 NU3

8 6 3 1411.65 0.004043 NU3

5 2 4 416.22 0.055572 NU3**

4 3 1 383.85 0.015576 NU3*

1

1

5 7 1985.83 4.215931 NUl

6 0 6 446.71 0.051494 NU3*

4 3 2 382.52 0.015487 NU3*

4 2 2 3;5.79 0.0215 NU1 +

1

1

3 9 1695.03 0.034735 NUl

5 1 5 1922 .86 0.030200 NU3***

3 0 3 136.77 0.000270 NU3*

7 1 6 2309.74 0.47 NUl***

5 1 4 399.46 0.000125 NU3

9 4 5 13'60.28 0.006880 NUl

7 0 7 2180.65 0.125531 NUl***

6 2 4 2211.21 0.157817 NU3***

7 2 5 782 .40 0.247061 NU3**

7 1 6 704,22 0.17 2NU2 +

9 8 2 2009,87 8.259078 NUl

9 8 1 2009,87 8.259079 NUl

6 1 5 542 .91 0.000758 NU3

11 4 8 1843.02 2. 124861 NUl

7 1 6 704.22 0. 154000 NU3*

7 0 7 5-86.26 0.001966 NU3
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm"' cm ~^ gm cm - nKJ tm1 1 1 1. 4073.87 11,7820 0, 0774 6 4

4074.66 0,0015 0,0645 5 5

4075.29 2 ,4512 0.0774 6 4

4075. 58 0,0336 0.0413 11 8

4075.58 0,1007 0.0412 11 8

4076.03 0 ,0044 0.0640 5 5

4076.40 0,0016 0. 0470 11 5 4076.85 0,0031 0.0794 7 2

4077.28 0,0015 0.0659 8 7

4077.34 0,0547 0.0481 12 7

4078. 14 0,0010 0.0607 9 4

4078.43 0,3292 0.0754 11 4

4078.45 0.3262 0.0656 7 5

4079.11 0,0182 0.0470 12 7

4079.42 25.2190 0.0841 8 4

4080.00 0.0028 0.0626 6 5 4080.20 0.4661 0.0822 6 5 4080.33 0,0086 0.0804 8 3

4081.28 9 ,3902 0.0794 7 2 4081.45 0,1728 0.0743 5 5

4083.61 0,0012 0.0405 11 9

4084,06 0,0039 0.0774 6 4

4084. 19 0,0290 0.0697 6 5 4084. 51 0,0077 0.0804 8 3

4084.87 3,8931 0.0645 5 5 4085. 56 0,0028 0.0650 9 2

4085.57 0,0022 0. 0378 9 9

4086.20 1 1 ,6938 0.0640 5 5 4086 .47 0,0062 0.0812 9 4

4086.81 0,0010 0.0442 12 6

4087.26 0,0083 0.0841 8 4

4087.38 0,0473 0.0744 7 4

4088.02 0,6971 0.0795 4 4

4088. 16 23,2913 C. 0804 8 3

4088.47 0,5215 0.0607 9 4

4088.58 0,2745 0.0722 10 3

4088.71 0,0384 0.0731 7 3

4088.74 0.0023 0.0655 7 7

4089.01 0.0012 0.0553 9 7

4089.20 0.0097 0.0679 6 5 4089,33 0.0023 0.0525 10 7

4089.97 0.0130 0.0369 11 9

4089,97 0.0391 0.0369 11 9

4090,32 0.0039 0.0569 8 7

4092,95 0.0014 0.0810 8 5

4093,01 0.2257 0.0836 7 5 4093,08 0,0810 0.0608 8 5 4093,24 0,0101 0.0494 10 4

4093, 54 1 ,4228 0.0650 9 2

4094,48 0,0054 0.0697 6 5 4096,71 0 ,0088 0.0744 7 4

4097,37 0,0071 0.0731 7 3

4099,36 0.0018 C.0679 6 5 4100,38 0.0013 0.0645 5 5

Kc J" E" L BAND

3 5 2 4 416.22 0.055572 NU3

0 4 3 1 383.85 0.015576 NU3*^^

2 5 1 5 326.64 0.0787 NU1 + 4 10 7 3 2054,40 7.018690 NUl

3 10 7 4 2054,40 7.018546 NUl

1 4 3 2 382 .52 0.015487 NU3**

7 1

1

2 10 1525.13 0.020871 NUl

5 6 0 6 2041 .76 0.051494 NU3***

2 7 4 3 931.22 0.003551 2NU2

6 1

1

6 5 2144,12 5.716270 NUl

6 8 1 7 882,93 0.269351 NUl*

7 10 3 8 1446,16 0.954846 NUl

3 7 1 6 704,22 0.002162 NU3

5 1 1 6 6 2142 ,69 5. 701369 NUl

4 7 2 5 782 .40 0,247061 NU3

1 6 0 6 446.71 0,000164 NUl

2 5 2 3 446.50 0,009072 NUl

5 7 1 6 704.22 0. 154000 NU3-«-^«- 5 6 0 6 446.71 0.051494 NU3

0 4 2 3 300.35 0.001619 NUl

3 1

1

7 4 2321 ,94 0.021839 NU3

3 5 2 4 2024. 17 0.055572 NU3-»^**

1 5 3 2 508,81 0.036022 NU3*

5 7 1 6 2309.74 0. 154000 NU3^«-«-*

0 4 3 1 383.85 0.015576 NU3

7 8 1 8 744. 16 0.122288 NUl*

1 9 7 2 1810.63 0.003527 NU3

1 4 3 2 382.52 0.015487 NU3

5 8 2 6 982.91 0. 240000 NU3*

7 12 3 10 1962 .55 0.040149 NUl

4 7 2 5 2392.58 0.247061 NU3***

4 6 2 5 552.92 0.073173 NU3*

0 3 0 3 136.77 0.000270 NU3

5 7 1 6 704,22 0. 154000 NU3-

6 8 1 7 882,93 0.269351 NUl

7 9 2 8 1080.38 0.380414 NUl

5 6 1 6 447.24 0.034900 NU3*

0 7 4 3 931 .22 0.000515 NUl

3 9 4 6 1340.89 0.006153 NUl

2 5 3 3 504.00 0.035127 NU3*

4 10 4 7 1581 .34 0.013111 NUl

3 10 8 2 2254.34 8.133537 NUl

2 10 8 3 2254. 34 8.133535 NUl

2 8 4 5 1 122 .72 0.002252 NUl

4 7 2 5 782.40 0.074366 NUl*

3 6 2 4 602 .77 0.028700 NUl

4 8 1 7 882.93 0.003922 NU3

7 10 1 10 1114,56 0.005517 NUl

7 8 1 8 744, 16 0.122288 NUl

1 5 3 2 508.81 0.036022 NU3**

4 6 2 5 552.92 0.073173 NU3**

5 6 1 6 447. 24 0.034900 NU3**

2 5 3 3 504.00 0.035127 NU3**

0 4 3 1 2005 .92 0.015576 NU3***

77
LINE HALF

FREQUENCY STRENGTH WIDTH J' J" Ka E" L BAND

cm ^ m — 1 LIN cm~'

ym cm atm.

4100.52 u , 008

1

0.0733 7 5 2 6 3 3 661.56 0,0638 52 NU3i^-

4101 . 49 0 .0038 0.0640 5 5 1 4 3 2 2004. 81 0,015487 3

4102.09 0.0537 0.0628 9 3 6 9 1 9 920.21 0,003124 NU3

4103 . 48 0.0012 0,0803 5 i^. 1 4 0 4 222.06 0. 00 1060 NU3-'*- 4104. 10 3 .1030 0,0812 9 4 5 8 2 6 982.91 0. 247000 NU3-

4104.77 14.5311 0 ,0697 6 5 1 5 3 2 508.81 0. 036022 NU3

4105.81 0.4528 0,0531 9 3 7 8 0 8 744,09 0, 116343 NU

1

4106 . 03 19.1581 0,0731 7 3 5 6 1 6 447 ,24 0 .034900 NU3-

4106.04 23 .6813 0 , 0 744 7 4 4 6 2 5 552.92 0,073173 NU3

4106.67 0.0112 0,0585 1

1

4 7 1

1

2 10 1525.13 0,013267 NU3

4107.03 0.7171 0,0810 8 5 4 7 2 5 782.40 0,074366 NUl

4107.40 0.0826 0,0590 8 4 5 8 0 8 744. 09 0,001991 NU3

4109.53 4.8438 0,0679 6 5 2 5 3 3 504,00 0,035127 NU3

4109. 54 0.0083 0,0572 7 5 2 7 0 7 586,26 0,000324 NUl

4110.49 0.1130 0,0709 6 5 1 5 2 4 416,22 0 ,005627 NUl

4110.93 0.0015 0,0733 7 5 2 6 3 3 661.56 0, 063852 NU3**

4111.86 0.0017 0, 0754 9 5 5 8 2 6 982.91 0.7281 NUl*

4111,87 0,0033 0,0625 1

1

3 8 1 1 0 1

1

1327. 14 0, 005168 NUl

4112 . 99 0,0013 0.0437 12 5 8 1 2 2 1

1

1774,74 0,018820 NUl

4113.45 0,0236 0.0684 7 5 3 6 3 4 648 ,97 0,058714 NU3^

4113.62 0.0161 0. 0760 8 5 3 7 3 4 842 .38 0, 105067 NU3*

4113.75 0.0063 0.0731 7 3 5 6 1 6 2042 . 77 0,034900 NU3**^i4114.15 0 .0045 0 .0756 7 A- 3 6 1 6 447 ,24 0, 0432 NUl^^

41 14. 43 0.1238 0.0558 9 5 5 9 1 8 1079 . 07 0 , 00 5298 NU3

4115.52 0.0186 0.0684 13 5 8 12 4 9 2124.98 1,92132 NUl

4116.52 0 ,0078 0.0744 7 4 4 6 2 5 2161.30 0,073173 NU3***

4118.86 0.0013 0.0525 10 4 7 9 1 8 1079 • 07 0.284777 NUl*

4120.36 0,0033 0.0670 10 5 6 9 2 7 1201.95 1,386 NUl*

4121.24 0 ,0048 0. 0697 6 5 1 5 3 2 2130.50 0,036022 NU3***

4121.35 4,0167 0.0733 7 5 2 6 3 3 661.56 0,063852 NU3

4123.24 0.0226 0 .0692 8 2 6 7 0 7 586.26 0, 0408 52 NU3*

4123.47 0,6004 0.0803 5 4 1 4 0 4 222 . 06 0.001060 NU3

4123. 57 0 .0044 0.0684 7 5 3 6 3 4 648 .97 0.058714 NU3**

4123.60 0.0084 0. 0691 8 4 5 7 2 6 709 . 60 0.084411 NU3*

4124.14 0 ,0030 0 . 0760 8 5 3 7 3 4 842 .38 0.105067 NU3**

4124.31 0,00 59 0.0 729 9 3 6 8 7 882.93 0. 139840 NU3*

4125 . 18 2,23 57 0.0756 7 4 3 6 1 6 447 . 24 0. 0432 NU1 + 4125 . 38 0,8625 0,0754 9 5 5 8 2 6 982.91 0.7281 NU1 + 4125 .46 0 ,0031 0.0768 9 5 4 8 3 5 1050 . 15 0. 169518 NU3*

4128.11 0,0075 0.0 540 6 6 0 5 4 1 610.35 0.015215 NU3*

4128.35 0,0025 0. 0535 6 6 1 5 4 2 610.12 0.015207 NU3*

4128.73 0,6267 0.0525 1 0 4 7 9 1 8 1079.07 0 .284777 NUl

4130.97 0,0245 n . 0696 ] 2 4 8 1

1

3 9 1695.03 0.720922 NUl

4131.01 0 . 0041 0.0692 8 2 6 7 0 7 586.26 0. 040852 NU3**

4132.74 0.0015 •0 . 0691 8 4 5 7 2 6 709.60 0. 08441

1

NU3**

4133.03 1 , 6544 0 . 0670 10 5 6 9 2 7 1201.95 1.386 NU1 + 4133.70 1 1 .8363 0.0684 7 5 3 6 3 4 648 .97 0.058714 NU3

4134. 66 8.0547 0 .0760 8 5 3 7 3 4 842 . 38 0, 105067 NU3

4137.35 0.0067 0 , 0648 8 3 6 7 1 7 586.48 0,036269 NU3*

4137.71 0.0384 0,0613 9 6 4 9 2 7 1201.95 0. 003008 NU3

4138.08 0 ,0037 0,0692 8 2 6 7 0 7 2180.65 0.040852 NU3***

4138 . 46 0.0010 0 , 0448 1

1

4 8 1

1

1 1

1

1327.14 0.004565 NUl

4138.79 11.2811 0.0692 8 2 6 7 0 7 586.26 0.040852 NU3

4138.90 0.0014 0,0733 7 5 2 6 3 3 2282.59 0.063852 NU3***

78
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm~i cm ' gm cnn-2cm 1 aim.

4139.25 0,0050 0,0681 8 5 4

4139,37 2 .9209 0,0729 9 3 6

4139. 46 0.0137 0,0642 8 6 3

4141.88 0.0159 0,0513 10 5 6

4141.89 4. 1963 0.0691 8 4 5

4142.08 0 .0045 0.0655 5 5 0

4142. 53 0 ,0024 0.0617 7 6 1 4142.77 0,0076 0.0561 10 6 5

4142.88 0,3617 0,0666 7 5 2

4145 . 30 0,0017 0.0552 8 5 3

4145 .35 0 .2388 0.0640 1

1

3 8

4145.95 0.0013 0.0648 8 3 6

4146.43 0.0039 0, 0783 6 4 2

4146.46 1 .5361 0,0768 9 5 4

4146.65 0 .0263 0,0664 7 6 2

4146.88 0.0937 0,0539 9 4 6

4148.79 0.1765 0.0536 10 2 8

4149.49 3 .7339 0. 0540 6 6 0

4149.65 0.0039 0.0684 7 5 3

4149. 72 1 .2455 0.0535 6 6 1 4149.78 0.0026 0,0589 7 6 1 4150.89 0.0081 0.0573 7 6 2

4152.61 0.0014 0.0691 8 4 5 4153.09 0.0026 0.0760 8 5 3

4153.36 2 .3648 0,0772 10 4 6

4154. 55 3.3475 0,0648 8 3 6

4155.00 0.0096 0,0517 1

1

6 6

4155 .96 0.5215 0,0457 10 3 8

4156.64 0.0010 0,0550 8 6 2

4157.07 0,0028 0.0660 6 6 1 4158.82 0,0061 0.0547 12 4 8

4159.06 0.0396 0.0578 10 3 7

4159.20 2.2350 0.0766 10 5 5 4159.29 2 .4705 0.0681 8 5 4

4159.74 0 .0027 0.0802 5 5 1 4161 . 59 0.0015 0. 0573 7 6 2

4163.50 0,0111 0.0623 9 4 6

4163. 53 0,1178 0,0573 1

1

5 7

4166.01 1 ,9787 0,0783 6 4 2

4166.34 0,0268 0,0625 6 5 1 4167 .64 0,0075 0. 0662 9 5 5

4168.22 0,0013 0,0540 6 6 0

4169.06 0,0494 0,0725 6 6 1 4169.63 0,0056 0.0628 8 6 2

4171,27 1 , 3364 0,0589 7 6 1 4172 ,30 4.0204 0,0573 7 6 2

4172,56 0.0713 0.0462 11 4 8

4173.18 0.0020 0. 0596 8 6 3

4173.59 0 .0012 0.0474 12 6 7

4173.64 0.0147 0.0478 11 5 7

4173.87 0.0165 0. 0662 6 6 0

4176.34 0.2879 0,0752 1

1

5 6

4177.29 0,0022 Cf,0485 9 6 3

4177,51 0.0014 0.0662 9 5 5

)" Kc E" L BAND

cm~i

7 3 5 816.72 0.084527 NU3*

8 1 7 882.93 0, 139840 NU3

8 2 6 982.91 0.001082 NU3

10 1 9 1293 ,04 0.005888 NU3

7 2 6 709.60 0. 084411 NU3

5 1 5 326.64 0.000013 NU3

7 1 6 704.22 0.000170 NUl

10 2 8 1438 .00 0.005881 NU3

6 2 5 552.92 0.011802 NUl

8 0 8 744. 09 0.000443 NUl

10 2 9 1293.66 0.316624 NUl

7 1 7 586.48 0,036269 NU3-^*

5 0 5 325,35 0,001931 NU3*

8 3 5 1050,15 0,169518 NU3

7 2 5 782 ,40 0.000253 NU3

9 0 9 920.18 0.001797 NU3

9 1 9 920.21 0. 108277 NUl

5 4 1 610.35 0.015215 NU3

6 3 4 2 271 .70 0.058714 NU3-«-**

5 4 2 610.12 0.015207 NU3

6 4 2 757.78 0.033963 NU3^

6 4 3 756.75 0.033870 NU3*

7 2 6 2318,53 0.084411 NU3-''«-** 7 3 4 2462 .87 0.105067 NU3***

9 2 7 1201.95 0. 185000 NU3-

7 1 7 586.48 0.036269 NU3

11 2 9 1690.70 0.008757 NU3

9 0 9 920. 18 0. 106449 NUl

8 1 7 882,93 0.000504 NUl

6 2 4 602 . 77 0.000032 NU3

12 2 11 1774,74 0.008389 NU3

10 1 10 1114.56 0,002006 NU3

9 3 6 1282 .92 0.261892 NU3

7 3 5 816.72 0.084527 NU3

4 0 4 222.06 0.000050 NUl

6 4 3 756,75 0.033870 NU3-''S-* 8 2 7 885.62 0.088564 NU3^-

10 2 8 1438 .00 0.963 NU1 +

5 0 5 325.35 0.001931 NU3

6 1 6 447 . 24 0.000048 NU3

8 3 6 1006 .12 0.109168 NU3*

5 4 1 2251 .86 0.015215 NU3^^*-«-

5 3 2 508.81 0.001286 NUl

7 4 3 931.22 0. 057059 NU3*

6 4 2 757.78 0.033963 NU3

6 4 3. 756.75 0.033870 NU3

10 1 9 1293.04 0.280036 NUl

7 4 4 927.77 0.056441 NU3*

12 2 10 1960.22 0.010688 NU3

1

1

1 10 1524.87 0.005757 NU3

5 3 3 504.00 0.001253 NUl

10 3 7 1538.23 0,359370 NU3

9 1 8 1079 .07 0.000971 NUl

8 3 6 1006 .12 0, 109168 NU3^4-^*-

79
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm 1 cm ' gm cm -2

cm * u Tm. 4179,75 0.0053 0 . 0648 10 3 7

4179.78 0.0030 0.0602 9 2 7

4179.79 0 .0861 0,0622 8 5 3

4181 . 44 5.5320 0,0623 9 4 6

4182.62 0.0598 0 ,0760 8 4 4

4185 . 19 0.0298 0,0771 7 6 2

4185.26 0.0018 0.0456 7 7 1 4187.38 3 ,7403 0 , 0662 9 5 5 4187.61 0,0084 0,0558 9 3 7

4188.59 0,0023 0,0 562 9 5 4

4189.45 0,0182 0,0630 13 4 9

4190. 12 0,0101 0,0497 10 4 7

4191.32 2 , 8424 0,0628 8 6 2

4192.35 0,0018 0,0623 9 4 6

4193.20 0 .0403 0.0717 5 5 0

4193 .80 0.2571 0 .0704 1

1

4 7

4194. 55 2.6213 0 .0648 10 3 7

4194. 60 0 .9548 0.0596 8 6 3

4195 . 58 0.0032 0.0601 9 6 4

4195.67 1 .4691 0,0602 9 2 7

4196.19 0,0016 0,0558 9 3 7

4196 . 43 0,0086 0.0587 7 5 2

4197 .03 0 , 0442 0.0488 12 8

4197 .14 0.0960 0.0801 8 6 3

4197 . 78 0.0875 0,0653 7 6 1 4198.86 0.0015 0,0677 10 6 4

4200.09 0.0021 0. 0563 1

1

7 5

4200.15 0,2592 0,072

1

12 5 7

4201.35 0,0205 0,0728 6 5 2

4201 .87 0,0225 0 , 0548 12 3 9

4202 . 18 0.1835 0 .0442 1

1

2 9

4202 .98 0 .0013 0 .0662 9 5 5

4204,77 4.2275 0.0558 9 3 7

4206 . 09 0.0276 0.0808 9 6 4

4206 ,35 0.0609 0 . 0404 1

1

3 9

4206,67 0.0014 0.0560 10 4 7

4206,92 0.0043 0,0 595 6 6 0

4207 ,53 0.3093 0.0457 7 7 0

4207 , 56 0.9278 0.0456 7 7 1 4207 . 79 0.0017 0.0493 8 7 1 4208 , 02 0.5267 0.0659 9 6 3

4208.15 0 .0013 0 • 0448 12 5 8

4214.07 0.0581 0.0781 10 6 5 4214. 12 0.4385 0 .0724 6 5 1 4215 . 50 0.0014 0.0558 9 3 7

4216.44 0.4221 0.0740 7 4 3

4216. 52 0.0032 0.0528 11 3 8

4216.94 1 . 5967 0.0601 9 6 4

4218 . 53 0.0645 0.0415 1

2

4 9

4218.65 0.5159 0.0616 1 0 5 6

4219.45 0.0031 0.0568 7 6 1 4221 .26 0.7306 0.0677 10 6 4

4222.85 0,0296 0.0630 8 6 2

4223. 15 0.1316 0.0603 9 5 4

J" E L BAND

cm-1

9 1 8 1079 .07 0.110021 NU3-

8 0 8 744,09 0. 034667 NU3^

7 2 6 709 .60 0.018297 NUl

8 2 7 885.62 0.088564 NU3

7 1 7 586 .48 0.006860 NUl

6 3 - 3 661.56 0.004975 NUl

6 5 2 888 , 60 0.014987 NU3*

8 3 6 1006. 12 0.109168 NU3

8 1 8 744. 16 0.033194 NU3*

9 0 9 920.18 0.000466 NUl

12 3 10 1962.55 0. 73907 NUl

10 0 10 1114,55 0.001525 NU3

7 4 3 931 .22 0.057059 NU3

8 2 7 2495. 18 0.088554 NU3*-^*

4 1 3 275,52 0.000091 NU3

10 2 8 1438 ,00 0. 196000 NU3-

9 1 8 1079 ,07 0.110021 NU3

7 4 4 927.77 0.056441 NU3

8 4 5 1122.72 0.082913 NU3*

8 0 8 744. 09 0.034667 NU3

3 1 8 744. 16 0.033194 NU3"'*-*

7 1 7 586.48 0.000093 NU3

11 2 9 1690,70 0.426841 NUl

7 3 4 842 .38 0. 013422 NUl

6 3 4 648 .97 0. 004557 NUl

9 4 5 1360.28 0. 124623 NU3*

11 3 8 1813.26 0.003273 NU3

11 3 8 1813.26 0.411017 NU3

5 0 5 325.35 0,000211 NUl

11 2 10 1525.13 0.278800 NUl

10 1 10 1114.56 0.097873 NUl

8 3 6 2630.21 0. 109168 f\lU3***

8 1 8 744. 16 0.033194 NU3

8 3 5 1050.15 0.032042 NUl

10 0 10 1114.55 0.097311 NUl

9 2 8 1080.38 0.087251 NU3*

6 2 5 552.92 0.000013 NU3

6 5 1 888.63 0.014988 NU3

6 5 2 888 .60 0.014987 NU3

7 5 2 1059.85 0,032814 NU3*

8 4 4 1131.76 0.085997 NU3

12 1 11 1774.60 0,005196 NU3

9 3 6 1282.92 0.071662 NUl

5 1 4 399 .46 0.000613 NU3

8 1 8 2337.70 0.033194 NU3***

6 0 6 446 .71 0.002241 NU3

11 1 11 1327.14 0.001419 NU3

8 4 5 1122.72 0.082913 NU3

11 1 10 1524.87 0.265959 NUl

9 3 7 1216.27 0.128613 NU3

7 2 6 709 .60 0.000062 NU3

9 4 5 1360.28 0. 124623 NU3

7 3 5 816.72 0.010619 NUl

8 2 7 885.62 0.022231 NUl

80
LINE HALF

FREQUENCY STRENGTH WIDTH J' Ka K, cm '

1 em » gm cm -2

i cm * atm.

4223. 17 0.0112 0.0725 1

1

6 6

4224. 24 0.0017 0.0460 13 3 10

4224.29 0.6933 0.0560 10 4 7

4224.63 0.0030 0.0633 9 7 3

4230 . 1 5 0.8683 0 . 0493 8 7 1 4230.35 0.2894 0 . 0489 8 7 2

4231.24 0.0991 0. 0684 1

1

6 5 4232.88 0.0160 0.0553 8 5 3

4233.37 0.0098 0.0662 13 5 8

4233 . 56 0.0043 0.0565 13 7 8

4234.53 0.0032 0.0511 10 2 8

4236. 10 0.0158 0.0657 12 6 7

4236 . 34 0.0088 0.0460 11 4 8

4236.92 0.0101 0.0533 8 6 2

4237.39 0 .0002 0.0573 10 5 5 4239.88 0 . 2443 0.0589 10 6 5 4239.99 0.1124 0.0678 12 6 6

4240 .00 0.2369 0.0717 7 5 2

4241 .78 0 .0040 0.0423 13 5 9

4242 .86 0.2336 0.0631 12 4 8

4243.89 0.0314 0 .0703 5 5 1 4249 .07 0.0079 0. 0642 7 5 3

4249 .95 0.0139 0.0668 13 6 7

4250.24 0.0635 0.0590 9 6 3

4250.62 0 .2534 0.0571 11 3 8

4250. 91 1.6355 0.0511 10 2 8

4251 .43 U .00 1

3

0 .0676 8 5 3

4251 .63 0 . 1789 0.0523 9 7 2

4252. 19 0.0550 0.0763 9 5

4252.35 0.5368 0.0 566 1

1

5 7

4252 .39 0.5391 0.0512 9 7 3

4254. 00 0.0195 0.0382 12 2 10

4255.71 0.5378 0.0482 10 3 8

4255.86 0.0585 0.0367 12 3 10

4256.26 0.0192 0 .0464 13 3 10

4257.57 0.0075 0.0 553 13 6 8

4259 . 40 0 .0023 0.0502 9 6 3

4259 . 55 0 .0604 0.0398 8 8 1 4259. 55 0,1810 0.0398 8 8 0

4262.18 0.0037 0.0610 7 7 1 4263.21 0.0111 0.0570 7 7 0

4264. 36 0.2809 0. 0574 11 6 6

4265.40 0.0059 0.0381 1 3 4 10

4269.82 0.6860 0 • 0499 1

1

4 8

4271.38 0.2618 0. 0548 10 7 3

4271 . 56 0 .0465 0.0612 10 5 6

4272.28 0.0024 0.0465 12 3 9

4272 .82 0 . 6444 0. 0676 8 5 3

4273.70 0.0882 0.0524 10 7 4

4275.56 0.5363 0.0696 8 4 4

4276.40 0.0023 0.0533 9 5 4

4278 .41 0.0015 0.0785 6 6 1 4280.86 0.0113 0.0543 10 6 4

4281.82 0.0170 0.0659 8 7 2

J" Kc E" L BAND

cm-i

10 3 7 1538.23 0. 147349 NUl

13 0 13 1806 .78 0.02938 NUl

9 2 8 1080.38 0.087251 NU3

9 3 6 1282 .92 0.000341 NU3

7 5 2 1059.85 0.032814 NU3

7 5 3 1059.65 0.032804 NU3

10 4 6 1616.51 0. 181046 NU3

8 1 8 744. 16 0.000125 NU3

12 3 9 2105.90 0.310600 NU3

12 5 7 2300.80 0.244900 NU3

9 0 9 920. 18 0.030629 NU3-^

1

1

3 8 1813.26 0.264753 NUl

11 0 11 1327.14 0.001260 NU3

8 2 7 885.62 0.000159 NU3

10 0 10 1114.55 . 0.000396 NUl

9 4 6 1340.89 0.112325 NU3

11 4 7 1899.06 0.265013 NU3

6 1 5 542 .91 0.00-2023 NU3

12 2 10 1960.22 0.40461 NUl

11 2 9 1690.70 0. 209597 NU3

4 1 4 224.83 0.000018 NU3

6 0 6 446.71 0.000443 NUl

12 4 8 2205.65 0.394450 NU3

8 3 6 1006 .12 0.019449 NUl

10 1 9 1293.04 0.091645 NU3

9 0 9 920.18 0.030629 NU3

7 1 6 704.22 0.004077 NU3*

8 5 3 1255.92 0.053971 NU3

8 1 8 744. 16 0.004551 NUl

10 3 8 1446. 16 0. 140157 NU3

8 5 4 1255. 16 0.053898 NU3

11 1 11 1327. 14 0.089480 NUl

9 1 9 920.21 0.030178 NU3

11 0 11 1327. 14 0.089303 NUl

12 2 11 1774.74 0.27474 NUl

12 3 9 2105 .90 0.37068 NUl

9 2 8 1080.38 0.000288 NU3

7 6 2 1216.20 0.014826 NU3

7 6 1 1216.20 0.014826 NU3

6 4 2 757.78 0.000981 NUl

6 4 3 756.75 0.000979 NUl

10 4 7 1581 .34 0. 142262 NU3

12 1 11 1774..60 0.25444 NUl

10 2 9 1293.66 0.082847 NU3

9 5 4 1477.31 0.079027 NU3

9 2 8 1080.38 0.0617 NU1 +

12 1 12 1557.91 0.001084 NU3

7 1 6 704.22 0.004077 NU3

9 5 5 1474.99 0.078635 NU3

7 0 7 586.26 0.001880 NU3

9 1 9 920.21 0.000130 NU3

5 1 4 399.46 0.000022 NUl

9 3 7 1216.27 0.029596 NUl

7 4 3 931 .22 0.003551 NUl

81
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq Kc

cm~' cm"'

gm cm"

2

otm.

4282.48 0.0492 0 • 0425 9 8 1 4282. 51 0 . 1476 0. 0424 9 8 2

4283.88 0.0015 0.0554 8 7 1 4285.27 0 .0057 0 .0579 8 7 1 4286.89 0 .0230 0.0685 6 5 2

4287.72 0.0539 0.0513 12 5 8

4287 . 88 0 .0033 0. 0474 10 6 4

4288.73 0.0350 0.0569 1

1

7 4

4290. 79 0.0303 0.0546 12 6 7

4294. 58 0. 1094 0.0504 1

1

7 5 4295.78 0.0199 0.0563 13 4 9

4298.14 0 .0051 0 . 0 708 9 7 3

4302 . 53 0.0012 0.0497 10 7 3

4302 . 83 0.0393 0.0584 12 7 5

4303.17 0.0172 0.0567 8 5 4

4303.84 0.0018 0.0728 7 6 2

4304.27 0.1885 0.0440 11 2 9

4304.45 0.0811 0. 0448 10 8 2

4304. 59 0.0271 0.0445 10 8 3

4305 .32 0.2121 0.0489 12 3 9

4305.46 0.0278 0. 0364 9 9 1 4305.51 0.0092 0.0364 9 9 0

4306.69 0.0179 0.0348 13 2 11

4306.71 0.5629 0.0421 11 3 9

4307. 18 0.0153 0.0578 9 7 2

4307.49 0.0059 0. 0342 13 3 11

4310.39 0.0101 0.0742 10 7 4

4313 . 34 0.0157 0.0665 6 6 0

4313 .68 0 .1226 0.0634 9 5 4

4315.72 0.0126 0.0513 12 7 6

4315.99 0.0139 0.0508 11 6 5 4316.70 0.0682 0. 0446 12 4 9

4317.97 0.0018 0.0753 11 7 5

4319.65 0.0196 0.0505 13 6 8

4322.40 0.0028 0.0737 12 7 6

4325.31 0.0108 0.0464 11 8 3

4325.84 0.0325 0.0454 11 8 4

4326.28 0.0167 0.0681 7 6 1 4327. 56 0.0022 0.0526 10 5 5 4327.73 0.0135 0.0638 1

1

5 6

4328.73 0.0068 0.0383 10 9 2

4328.73 0 .0204 0.0384 10 9 1 4329.74 0 ,0045 0.0755 10 4 6

4329.78 0.0033 0.0555 10 7 3

4329.79 0.0362 0.0464 13 5 9

4335 . 30 0.0082 0.0627 8 6 3

4335.43 0.0755 0.0644 7 5 3

4340 .14 0.0874 0.0682 8 6 2 4342 . 92 0.0546 0.0654 9 4 5 4343.62 0.0038 0.0631 6 6 1 4345.08 0.0111 0.0474 12 8 4

4345 .85 0.0032 0 . 0436 10 1 0

4346.51 0.0037 0.0462 12 8 5 4349.01 0.0020 0.0490 8 8 1

J Kc c. L

\ cm-1

8 6 2 1411.68 0.032025 NU3

8 6 3 1411.65 0.032024 iMU3

8 3 6 1006. 12 0. 000044 NU3

7 4 4 927 .77 0.003511 NUl

5 1 5 326 .64 0.000066 NU3

1

1

3 9 1695.03 0. 143644 NU3

10 2 9 1293 .66 C. 000402 NU3

10 5 5 1724.72 C. 108914 NU3

11 4 8 1843.02 0. 169033 NU3

10 5 6 1718.77 C. 107152 NU3

12 2 10 1960.22 0.185870 NU3

8 4 4 1131 .76 0.008626 NUl

10 3 8 1446.16 0.000310 NU3

1

1

5 6 1999.02 0. 145917 NU3

7 0 7 586.26 0. 000639 NUl

6 1 5 542 .91 0.000161 NUl

10 0 10 1114.55 0. 027627 NU3

9 6 3 1631.41 C. 051960 NU3

9 6 4 1631.27 0.051950 NU3

11 1 10 1524.87 0.080345 NU3

8 7 2 1590 .74 0.014704 NU3

8 7 1 , 1590.74 0.014704 NU3

12 1 12 1557.91 0.08639 NUl

10 1 10 1114.56 0.027489 NU3

8 4 5 1122.72 0.008300 NUl

12 0 12 1557.91 0.08609 NUl

9 4 5 1360.28 0.017923 NUl

5 2 3 446 . 50 0.000027 NU3

8 1 7 882.93 0.005631 NU3

1

1

5 7 1985.83 0. 139005 NU3

10 3 8 1446. 16 0.037991 NUl

1

1

2 10 1525.13 0.077267 NU3

10 4 6 1616.51 0.035256 NUl

12 4 9 2124.98 0. 181000 NU3

1

1

4 7 1899.06 0.068678 NUl

10 6 4 1875.53 0.074997 NU3

10 6 5 1875 .00 0.074947 NU3

6 , 2 4 602 .77 0.000189 NU3

10 1 10 1114.56 0.000109 NU3

10 2 9 1293 .66 0.017174 NUl

9 7 3 1810.63 0.031444 NU3

9 7 2 1810.63 0.031445 NU3

9 1 9 920.21 0.002627 NUl

9' 4 6 1340.89 0.015023 NUl

12 3 10 1962 .55 0. 133420 NU3

7 1 6 704.22 0.000543 NUl

6 1 6 447.24 0.000130 NU3

7 2 5 782 .40 0. 000806 NU3

8 0 8 744.09 0.001245 NU3

5 2 4 416.22 0.000017 NU3

11 6 5 2144. 12 0. 101574 NU3

9 8 1 2009.87 0.014608 NU3

11 6 6 2142.69 0.101336 NU3

7 5 2 1059.85 0.000796 NUl
LINE HALF

FREQUENCY STRENGTH WIDTH J' Kq

cm ' cm ' gm cm -2

cm ' atm.

4349.39 0.0086 0.0510 14 4

4350.78 0.0033 0.0450 14 6

4351. 15 0.0083 0.0398 11 9

4351.15 0 .0028 0.0399 11 9

4353. 16 0.0051 0.0522 11 7

4356.13 0.1801 0.0389 12 2

4356.22 0.0015 0.0496 12 6

4356.87 0.0326 0.0655 9 6

4357.49 0.0599 0.0379 12 3

4357.52 0.0016 0.034 14 2

4358.02 0.0049 0.034 14 3

4358. 14 0.0540 0.0438 13 3

4362. 97 0.0028 0. 0481 13 8

4363.05 0.1431 0.0597 10 5

4364.20 0.0030 0.0524 9 5

4364.24 0.1541 0.0402 13 4

4366.67 0.0021 0.0457 13 8

4369.22 0.0017 0.0549 1

1

10

4370.08 0.0027 0.0495 9 8

4372.96 0.0039 0.0410 12 9

4373.01 0.0013 0.0390 12 9

4373.31 0.0024 0.0549 9 6

4374.44 0.0023 0.0440 14 5

4376. 13 0.0264 0.0617 7 6

4379. 59 0.0721 0.0625 10 6

4388,29 0.0021 0.0559 10 8

4388.87 0.0010 0.0662 12 5 4389.53 0.0177 0.0592 8 5 4407.00 0.0170 0.0357 13 2

4407. 50 0.0510 0.0350 13 3

4408.80 0,0135 0.0410 14 3

4409.75 0.0118 0.0578 1

1

6

4410.03 0.0028 0.0728 11 4

4411.21 0.0012 0.0504 11 8

4411.92 0.0048 0.0370 14 4

4412.77 0.0105 0.0586 8 6

4*414.80 0.0037 0.0497 10 5 4417.92 0.0042 0.0481 10 6

4421.53 0 .0134 0.0571 11 5

4435. 13 0.0399 0.0617 10 4

Kc

II J Kq Kc E L BAND

cm-1

10 1 3 2 11 2246 .98 0. 160530 NU3

9 13 4 10 2426.22 0. 186890 NU3

3 10 7 4 2054 . 40 0.050502 NU3

2 1 0 7 3 2054.40 0.050503 NU3

4 10 4 7 1581 .34 0.025914 NU 1 10 1

1

0 1

1

1327 . 14 0.025215 NU3

6 1 1 3 9 1695 . 03 0.041150 NUl

3 8 2 6 982.91 0.002446 NU3

10 1

1

1 1

1

1327 . 14 0.025171 NU3

12 13 1 13 1806.78 0.08004 NUl

12 13 0 13 1806.78 0.07993 NU 1 10 12 1 1

1

1774,60 0.074330 NU3

5 12 6 6 2437.56 0. 150080 NU3

5 9 1 8 1079 . 07 . 0 . 00 5774 NU3

5 8 0 8 744 , 09 0.000727 NUl

10 12 2 11 1774 . 74 0.070610 NU3

6 12 6 7 2433 .85 0.037850 NU3

2 10 8 3 2254 . 34 0.030999 NU3

1 8 5 4 1255.16 0.002788 NUl

3 1

1

7 4 2321.94 0.072157 NU3

4 1

1

7 5 2321.89 0.072150 NU3

4 8 1 7 882.93 0. 00 1 147 NUl

10 1 3 3 1

1

2248 .16 0,129110 NU3

2 6 2 5 552.92 0.000077 NU3

4 9 2 7 1201 .95 0.00 5348 NU3

3 9 5 4 1477 .31 0.006528 NUl

7 1

1

2 10 1525.13 0.011578 NUl

4 7 1 7 586.48 0. 000182 NU3

1

1

12 0 12 1557.91 0.023180 NU3

1

1

12 1 12 1557.91 0.023120 NU3

11 13 1 12 2042 .33 0. 067400 NU3

5 10 2 8 1438 .00 0.008540 NU3

7 1 0 1 10 1114.56 0.001448 NU 1 3 1 0 5 6 1718.77 0.012538 NU 1 1

1

1 3 2 12 2042 . 38 0.065890 NU3

3 7 2 6 709 .60 0. 000198 NU3

6 9 0 9 920.18 0. 000705 NU 1 5 9 1 8 1079.07 0.001773 NUl

6 10 1 9 1293.04 0.004657 NU3

6 9 0 9 920. 18 0.000715 NU3

83

Part II. Atlas of Computed Transmission Spectra for

2.7/i U,0 Band

David M. Gates, Robert F. Calfee, and David W. Hansen

Theoretical transmission spectra of the 2.7m atmospheric water vapor band at infinite spectral resolution have been determined for specific values of pressure, temperature, and

water vapor concentration. A triangular slit function has been applied to the theoretical

spectra to show the effect of slit width upon the resolution of an actual instrument. Both

the theoretical and "degraded" spectra are displayed in graphic form.

1. Introduction

The transparency of the Earth's atmosphere to

infrared radiation of various frequencies is of great

importance to astronomers, meteorologists, atmospheric physicists, commvmications engineers, ecologists, and others. The infrared spectral region covers a broad wavelength span from 7000 A or

0.7m to 1000m or 1 mm, and a frequency span

from 14,300 cm-H4.28X10"c/s) to 10 cm-^S-OX

10"c/s). The infrared region spans 10.5 octaves

compared with the visible which spans less than

1 octave. If the atmosphere were transparent

this would present a magnificent opportunity for

communication beyond the very crowded radiofrequency region and beyond the very narrow

optical region of the electromagnetic spectrum.

Both fortunately and unfortimately, the Earth's

atmosphere possesses many strong and broad

absorption bands throughout the infrared spectrum due to water vapor, carbon dioxide, ozone,

and weaker absorption bands arising from methane, nitrous oxide, heavy water, and other very

minor constituents. Sunlight is absorbed by these

gases in the atmosphere and the atmosphere re- radiates this heat toward space and toward the

ground. The climate of the Earth is greatly

modified by this absorbed radiation. Without

this warmth the Earth's surface would become

intensely cold at night, and without the shielding

affect of the atmosphere from the infrared solar

radiation the daylight side would become very

much hotter.

The location of many of the absorption bands

at infrared frequencies are seen in figure 1, which

represents a direct recording of solar radiation

transmitted by the atmosphere. Although the

absorption bands are numerous, there are "windows" between some of these bands where radiation passes relatively unattenuated through the

atmosphere. The best window of the entire

infrared spectrum occurs at 11.08 microns, but

other windows are good, particularly when the

path length is not too great. A detailed analysis

of the spectrum shown in figure 1 giving attenuation coefiicients as a function of the frequency

has been given by Gates [1960] and by Gates and

Harrop [1963j.

The absorption spectrum is actually very much

more complex than it would appear to be in figure

1. Each absorption band when fully resolved is seen to be comprised of many hundreds of individual absorption lines. A typical segment of the

highly resolved absorption spectrum is shown in

figure 2 as taken from the Migeotte Atlas [1956].

A thorough understanding of the infrared transmission by the atmosphere involves a detailed

analysis of the high resolution spectrum. This

requires that one deal with each and every line in

the spectrum and with the simultaneous collective

effect of the wings of many lines on the transmission of the atmosphere at any specific frequency.

The precise nature of the observed spectrum will

depend upon the instrument used for the observation, the spectrum being degraded by the influence

of the slit or instrument factor. Before a careful

analysis can be made of the spectral transmission

as observed, it is first necessary to establish in

detail the theoretical spectral transmission, which

would be recorded with an instrument of infinite

resolving power. This requires that one calculate

the detailed absorption spectrum for each of the

major absorbing molecules present in the Earth's

atmosphere. Since water vapor is one of the most

important constituents, these calculations have

been performed for this molecule first. Calculations have been made of the line positions, line strengths, and line half-widths of the

water vapor spectrum from the quantum mechanical analysis of the asymmetric rotator. These

results have been presented in tabular form by

Gates, Calfee, Hansen, and Benedict [1963] for

the frequency span 2857 to 4444 cm"'.

85
2. Transmission

The monocliromatic transmission at a frequency

I', of m g cm~^ of absorbing gas at a constant

pressiire and temperature is

r^(m)=exp (—hm) (1)

where kv is the monochromatic absorption coefficient.

Each absorption Hne is affected by collisions

which shorten the natm-al lifetime of excited

vibrational states. The following Lorentz formula

is taken to reasonably represent the spectral line

shape which gives the monochromatic absorption

coefficient in the following form:

where i^o is the frequency of the line center, 5* is the

Une strength which depends upon temperature

according to

s=s.(|»)"%xp[=f:-'(%if)]

a is the half-width of the line which depends

upon pressure and temperature in the following

manner

where P/Po is the total pressure of the gas in

atmospheres, T the absolute temperature, and n

depends upon the nature of the broadening gas

and the frequency of the transition. For N2-

H2O collisions, Benedict and Kaplan [1959] show

n=0.62 to be a good representative value. Here

5^0 and ao refer to the strength and half-width,

respectively, calculated at a reference temperature Tq.

The line strength, S, is composed of vibrational

and rotational contributions, Sr and S^, determined by

Qr "0

The central frequency of the band is vq. The

rotational factor Sr for a particular rotational

transition is Sr=Lg exp (-E"/kT)

where L is the rotational transition strength defined to be the sum of the squares of the magnitude

of the direction cosine matrix elements evaluated

for the asymmetric rotator. A full discussion of

the evaluation of L for a rigid asymmetric rotator

has been given by Cross, Hainer, and King [1944].

Schwendeman and Laurie [1958] have published

a very useful table giving values of i as a function

of the asymmetry parameter, k, for all transitions

up to J=12. Wacker and Pratto [1963] have

extended the computations of L to higher J values.

For the ground state of H2O, k=—0.4377 was

used for the present computations.

The statistical weighting factor g depends upon

the symmetry of the ground energy level E"

[Townes and Schawlow, 1955].

The rotational partition fimction is given by

Qr=i: (2J+1)^ exp {-E"lkT).

J

The vibrational transition probability, S^, is common to aU lines in a band.

However, the transmission at any frequency in

the spectrum depends not only on the shape, halfwidth, and strength of the nearest line, but is also

influenced by the wings of many dozens of lines on either side. Therefore, to obtain the actual

absorption coefficient at any frequency, it is necessary to sum the influence of many lines as follows

k{v)=JZh=^^r-. ^. (5)

77 I7 TT [(f-J'o) +0! ] The transmission for a given pressure, temperature, and water vapor concentration is now given

as a function of the frequency v,

T(v)=exp [-k{v)m]. (6)

The total absorption across an entire band is invariant to the spectral slit width of the instrument [Nielson, Thornton, and Dale, 1944]. For

this reason the total band absorption is often

given by experimentalists rather than the specific

absorption within a narrow spectral interval.

The total band absorption is given by

A= f"' A(v)dv= f"' [l-T{v)]dv (7) J"! J"!

where vi and V2 are the frequency limits for the band.

3. Computational Procedure

It was desired to compute the transmission as a function of the frequency across a definite frequency interval for a given pressure, temperature,

and water vapor concentration. To avoid any

end effects, the computation was extended to

include the strong lines out to 150 cm~^ on either

side of the interval selected. Starting with the

first point of the interval, the transmission was | computed by calculating directly the contributions

of all lines by means of the Lorentz line shape

formula. This was a straight siun of the k^'s at 1 this position. The frequency value was then

86
increased by a fixed increment, 0.01 cm~\ and the

transmission again calculated. When the point

came within 0.05 cm~^ of a line center, the increment was decreased to 0.0005 cm~' in order to

gain the full influence of the line on the calculations. Furthermore, at the position of each line

the influence of all other lines was summed up to

give an added effective strength to the single line

absorption coefficient. By using a coarse increment when far from line centers and a fine increment when close, a marked saving of computer

time was realized. After calculating the transmissions throughout the total interval, the total

absorption was calculated using Simpson's rule,

taking into account the two sizes of step intervals.

The computed theoretical water vapor spectra

for the frequency interval 3500 to 4000 cm"' are shown in figure 3 for a pressure of 0.1 atmosphere

and figure 4 for a pressure of 1.0 atmosphere at a temperature of 287.7 °K. The water vapor concentration was changed in certain sections of the

spectrum in order to display the line structure to

better advantage. The values of water vapor

concentration are indicated on each plate in fig- ures 3 and 4. The necessary data for computation are the

pressure in atmospheres, the water vapor concentration in precipitable centimeters, and the

absolute temperature along with the line positions,

line strengths, half-widths, and energy values

of the initial state.

4. Degraded Spectra

A spectrometer scanning an absorption spectrum

will not record it with the sharp detail of the

natural line shape but will degrade the spectrum

because of finite slit widths and limited dispersion

of the grating or prism. Since all observed spectra

are of this degraded nature to various degrees,

it is desirable to modify the theoretical spectrum

described earlier with a slit function or instrument

factor. Several authors have discussed slit factors,

including Dennison [1928], Nielsen, Thornton, and

Dale [1944], Kostkowski and Bass [1956], and

Rautian [1958].

The slit function, p{v), is defined according to

the degraded transmission T..^ recorded by the

spectrometer at a frequency, Vi, as follows:

where T„ is the theoretical transmission at infinite

resolving power at any frequency v, Vi is the frequency at the center of the spectral interval

being momentarily scanned by the exit slit, and

a is the spectral slit width (defined as one-half of

the total frequency span passed by the spectrometer slits)

.

Various approximations to the slit function can be derived such as a Gaussian distribution, a

trapezoidal type of distribution, and a triangular

fimction. The simplicity of the triangular function and the fact that it represents reasonably

well the slit distortions across the central maximum

make it attractive for computational purposes.

The triangular slit function was used in the following form

p'v)=a-\v-Vi\. (9)

To compute the degraded spectrum from the

theoretical spectrum, the triangle slit function

was superimposed upon the theoretical spectrum.

Then the average transmission was calculated

across the frequency span passed by the slit. The slit fimction was shifted across the spectrum

by increments of approximately 0.2 to 0.4 cm"',

depending upon the slit width used, and at each

position the average transmission across the slit was computed, using (8). The averaging process

within the spectral interval was calculated in

steps of 0.05 cm"'.

The theoretical water vapor spectra of figures

3 and 4 covering the frequency range from 3500

to 4000 cm"' are shown in degraded form in

figures 5 to 7. The degraded spectra were calculated for spectral slit widths, 0.5 cm"' and 1.0

cm"', or a full slit span of 1 cm"' and 2 cm"'.

Again pressures of 0.1 and 1.0 atmosphere were

used at a temperature of 287.7 °K.

Within the figures on a single plate the effect of

the difference in water concentration can be seen. By a comparison of figures 5 and 6, the pressure

effect on the spectrum can be observed since the

same spectral slit width was used for each. Figures

6 and 7 show the effect of a change in slit width

at constant pressure. These figures are presented

as examples of the type of theoretical analysis

possible.^ Given any pressure, temperature, and

water vapor concentration, the theoretical spectrum can be computed. With additional information about spectral slit conditions, this theoretical

spectrum can be degraded to any degree.

Figure 8 shows a small portion of the spectrum

degraded by a triangular half slit width of 0.05

cm"'. As narrower slit widths are used (below

about 0.1 cm"') the triangular function becomes

more and more inadequate as a slit function.

This figure is included to show the type of spectral

structm-e to be expected from a high resolution

spectrometer. For a more correct presentation of

the narrow slit spectrum, a more refined slit function, e.g., a Gaussian function, could be used.

2 Spectral data for any specific region in the 2.7ft H2O band and any conditions of pressure, temperature, and slit conditions can be furnished in either graphic form or as numerical tables.

87
The authors particularly thank W. S. Benedict

of Johns Hopkins University and the National

Bureau of Standards, Washin2;ton, D.C, for his

invaluable assistance in providing the necessary

information for determining the line positions,

strengths, and haK-widths required for the above

analysis. The authors acknowledge the assistance

of Charles C. Rimner in preparing the figures.

5. References

Benedict, W. S., and L. D. Kaplan (1959), Calculations of

line widths in H2O — N2 collisions, J. Chem. Phys. 30,

388—399

Cross, Paul C, R. M. Hainer, and Gilbert W. King (1944),

The asymmetric rotor, J. Chem. Phys. 12, 210-243.

Dennison, D. M. (1928), The shape and intensities of

infrared absorption lines, Phys. Rev. 31, 503-519.

Gates, D. M. (1960), Near infrared atmospheric transmission of solar radiation, J. Opt. Soc. Amer. 50, 1299-1304.

Gates, D. M., Robert F. Calfee, David W. Hansen, and

W. S. Benedict (1963), Line positions, strengths, and

half-widths for water vapor bands vi, 2 V2, and in the

interval 2857 to 4444 cm-i, NBS Monograph No. 71,

part I. Gates, D. M., and Walter J. Harrop (1963), Infrared trans- mission of the atmosphere to solar radiation, Appl.

Optics, 3, No. 9, 887-898.

Kostkowski, H. J., and A. M. Bass (1956), Silt function

effects in the direct measurement of absorption line half- widths and intensities, J. Opt. Soc. Amer. 46, 1060-1064.

Migeotte, M., L. Neven, and J. Swensson (1956), The solar

spectrum from 2.8 to 23.7 microns. Part I, Photometric

Atlas, University of Liege.

Nielsen, J. Rud, V. Thornton, and E. Brock Dale (1944),

The absorption laws for gases in the infrared. Rev. Mod.

Phys. 16, 307-324.

Schwendeman, R. H., and V. W. Laurie (1958), Tables of

line strengths, Pergamon Press, Inc., New York, 39 pp. Townes, C. H., and A. L. Schawlow (1955), Microwave

spectroscopy, McGraw-Hill Book Company, Inc., New

York, 102.

Wacker, Paul F., and Marlene R. Pratto (1963), Micro- wave spectral tables. Vol. II, Line strengths of asymmetric rotors, NBS Monograph No. 70.

88
707-944

O - 54 - 7 89

p= 0.1 atm. w = 0.001 pr cm HjO

1—I r rm rn n

90

70

60

o

CO

cn

CO<

^ 50

i 40

LlI

Q: 30 Q.

20

10

OL

3550 40 30 20 FREQUENCY cm"'3500

p = ai atm. ryra

w = 0.010 pr cm HgO

Tl

Km 90 n

2

g

CO

70 —

60 —

<

E 50

^ 40

LlJ O

cc 30

20

10 —

^

/n

3550 40 30 20 3500 FREQUENCY cm"

Figure 3. Computed high resolution theoretical spectra for the frequency range 3500 to 4000 cm — ^ at a pressure of 0.1 atmosphere and at concentrations of 0.001 and 0.01 cm of precipitable water vapor for a temperature of 287.7 °K.

It should be noted that for the range 3950 to 4000 cm-' in the wing of the band where the absorption is weak, the concentrations used are 0.01 and 0.10 cm of precipitable water vapor.

91
P=0.latnn. w = O.OOi pr cm HgO

3600 90 80 70 60 3550 FREQUENCY cm''

FiGUEE 3.—Continued

92
p = O.I atm. w = 0.001 pr cm HgO

FREQUENCY Cm"'

FiGUEB 3.—Continued

93
P=O.I atm. w = 0.001 pr cm HgO

FREQUENCY cm''

Figure 3.—Continued

94
P = O.I atm. w =0.001 pr cm HgO

3750 40 30 20 10 3700 FREQUENCY cm"'

P = O.I atm. w = 0.010 pr cm HjO

FREQUENCY cm"'

FiGUBB 3.—Continued

95
P=O.I atm. w =0.001 pr cm HgO

FREQUENCY cm

FiGtJHB 3.—Continued

96
P=0.latm. w = 0.001 pr cm H2O

FREQUENCY cm"'

Figure 3.—Continued

97
P = 0.iatm. w = 0.001 pr cm HgO

3900 90 80 70 60 3850 FREQUENCY Cm''

p = 0.l atm. w = 0.010 pr cm

3900 90 80 70 60 3850 FREQUENCY cm"'

Figure 3.—Continued

98
P= 0.1 atm. w = 0.001 pr cm HgO

wnv nn rvYY ^

90

i 70

w 60 z

<

^ 50«-

2 40|f—

UJo

P=, 301—

20 —

10

03950 40 30 20 FREQUENCY cm''

3900

P = 0.1 atm.

100

90

80

70

60

w = 0.010 pr cm HjO

hft-

<

£ 50

5 40

UJo

£ 30

20

Ol_

3950

n

40 30 20 FREQUENCY cm"'

3900

FiGUEE 3.—Continued

99
P=0.l atm, w= 0.010 pr cm HgO

4000 90 80 70 60 3950 FREQUENCY cm''

P=0.latm. w= 0.100 pr cm HgO

4000 90 80 70 60 3950 FREQUENCY cm"'

Figure 3.—Continued

100
P = 1.0 atm w = 0.001 pr cm H2O

3500 FREQUENCY Cm"

P= 1.0 atm. w = 0.010 pr cm HgO

3500 FREQUENCY cm

Figure 4. Computed high resolution theoretical spectra for the frequency range 3500 to 4OOO cm—^ at a pressure of 1.0 atmosphere and at concentrations of 0.001 and 0.01 cm of precipitable water vapor for a temperature of 287.7 °K.

It should be noted that for the range 3950 to 4000 cm-i in the wing of the band where the absorption is weak, the concentrations used are 0.01 and 0.10 cm of precipitable water vapor.

101
P=i.Oatm. w= 0.001 pr cm HjO

3600 90 80 70 60 3550 FREQUENCY cm"'

P=l.Oatm. " w = 0.010 pr cm HgO

FREQUENCY Cm

FiGUBE 4.—Continued

102
103
P= 1.0 atm. w = 0.001 pr cm HgO

FREQUENCY cm"'

Figure 4.—Continued

104
p = 1.0 atm. w = 0.001 pr. cm H2O

.0 atm.

30 20 FREQUENCY cm''10 3700

w = 0.010 pr cm H2O

03750 30 20 FREQUENCY cm"'

Figure 4.—Continued

707-944 O - 64 - 105
P= 1.0 atm.

100 w = 0.001 pr cm HgO

w 60 <

£ 50

5 40 O

P= 30

SOTO

20 —

0L_

3800

A

90 70 FREQUENCY Cm'60 3750

P= 1.0 atm. w = 0.010 pr cm H2O

FREQUENCY cm

Figure 4.—Continued

106
p = 1.0 atm. w = 0.001 pr. cm HgO

FREQUENCY cm"!

Figure 4.—Continued

107
p = 1.0 atm w = 0.001 pr. cm HgO

80 70 FREQUENCY cm"'

3850

p = 1.0 atm. w.= 0.010 pr. cm HjO

FREQUENCY cm"'

FiGUBE 4.—Continued

108
p = 1.0 atm. w = 0.001 pr. cm HgO

p = 1.0 atm.

FREQUENCY cm" w = 0.010 pr. cm HjO

03950 30 20 FREQUENCY cm"'

3900

Figure 4.—Continued

109
P=i.Oatm. w = 0.010 pr cm H2O

FREQUENCY Cm''

Figure 4.—Continued

j

110
p= 0.1 atm UPPER CURVE ; w = o.ooi pr. cm HgO lower curve: w = QOIO pr. cm HgO SPECTRAL SLIT (2a) = 1 .0cm'

30 20 FREQUENCY cm"'3500

3550 FREQUENCY cm

Figure 5. Computed degraded water vapor transmission spectra for the frequency range 3500 to 4000 cm—^ at a pressure of

0.1 atmosphere, at concentrations of 0. 001 and 0.01 cm of precipitable water vapor, for a temperature of 287.7 °K, and at a

full spectral slit (triangular) span of 1.0 cm — ^.

Ill
p = 0.latm UPPER CURVE: w = 0.001 pr. cm HgO LOWER CURVE- w = 0.010 pr. cm HgO SPECTRAL SLIT (2a) = 1.0 cm"'

FREQUENCY cm"'

FREQUENCY cm''

FiGUHE 5.—Continued i

I

I

I

I

!

i

I

112
p =0.1 atm UPPER curve: w = 0.001 pr. cm H^O LOWER CURVE: W =0.010 pr. cm Hp SPECTRAL SLIT (2a) = 1.0 cm"'

FREQUENCY cm'

3fi00 90 80 70 6 0 3750 FREQUENCY cm"'

Figure 5.—Continued

113

^07-944 O - 64 - 9 .
p = 0,latnn UPPER CURVE^ w = 0.001 pr cm HjO LOWER CURVE^ w = 0.010 pr cm HjO SPECTRAL SLIT (20) = 1.0 cm'l

3900 90 80 70 60 3850 FREQUENCY cm''

FiGUEE 5.—Continued

114
p = 0.1 atm UPPER CURVE: w = 0.001 pr. cm HgO LOWER CURVE: w = 0.010 pr. cm HgO SPECTRAL SLIT (2a) = 1.0 cm"'

Q: 30 —

20 — —

10— u _

I I I I

11

"3950 40 30 20 10 3900 FREQUENCY cm '

4000 9 0 8 0 TO 60 3950 FREQUENCY cm"'

Figure 5.—Continued .

115
p=I.Oatm UPPER CURVE: w = 0.001 pr. cm LOWERCURVE: W = 0.010 pr. cm HgO SPECTRAL SLIT (2a) = 1.0 cm-i

3600 90 80 70 60 3550 FREQUENCY cm"'

Figure 6. Computed degraded water vapor transmission spectra for the frequency range 3500 to 4000 cm—^ at a pressure of

1.0 atmosphere, at concentrations of 0.001 and 0.01 cm of precipitable water vapor, for a temperature of 287.7 °K, and at a

full spectral slit (triangular) span of 1.0 cm — ^.

116
p= 1.0 atm UPPER CURVE: w = 0.001 pr. cm H^O LOWER CURVE: w = 0.010 pr. Cm HgO SPECTRAL SLIT (20) = LO Cm"'

3700 90 80 ,70 60 3650 FREQUENCY cm '

FiGUBB 6.—Continued

117
118
119
p=I.Oatm UPPER CURVE: W = 0.010 pr. cm HgO LOWER CURVE: W = 0.100 pr. cm HgO SPECTRAL SLIT (2a) = 1.0 cm''

3950 40 30 20 10 3900 FREQUENCY cm"'

4000 90 80 70 60 3950 FREQUENCY cm"'

FiGUEE 6.—Continued

120
p=I.Oatm UPPER CURVE: w = 0.001 pr. cm HaO LOWER CURVE: W = 0.010 pr cm HgO SPECTRAL SLIT (2a)=2.0 Cm"'

3550 40 30 20 FREQUENCY cm"'

3500

80 70 FREQUENCY cm''

60 3550

Figure 7. Computed degraded water vapor transmission spectra for the frequency range 3500 to 4000 cm — ^ at a pressure of

1.0 atmosphere, at concentrations of 0.001 and 0.01 cm of precipitable water vapor, for a temperature of 287.7 °K, and at a

full spectral slit (triangular) span of 2.0 cm—^.

121
p=I.Oatm UPPERCURVE: W = 0.001 pr. cm HjO LOWER CURVE: W = 0.010 pr. cm HgO SPECTRAL SLIT(2a)=20cm'

FREQUENCY cm"'

Figure 7.—Continued

122
p= 1.0 atm UPPER CURVE: w = 0.001 pr. cm HgO LOWER CURVE: W = 0.010 pr. cm HjO SPECTRAL SLIT (2a) =2.0cm''

100

1

\ \ 1 1

1

FREQUENCY Cm '

Figure 7.—Continued

X23
124
125
p = 0,1 atm. SPECTRAL SLIT (2a) = 0.1 Cm

w = 0001 pr. cm HgO

CO

CO

<

LiJ

tr

LlI Q.

3550

p = 0.1 atm.

40 30 20 FREQUENCY cm"'

3500

w = 0.010 pr. cm HgO

1 n

90

to^ 60 <

e 50

LUO

q:

UJ

CL

40

30

20

3550 40 30 20 3500 FREQUENCY cm"

Figure 8. Computed degraded water vapor transmission spectra for the frequency range 3500 to 4000 cm— ^ at a pressure of

0.1 atmosphere, at concentrations of 0.001 and 0.01 cm of precipitable water vapor, for a temperature of 287.7 °K, and at a

full spectral slit {triangular) span of 0.1 cm—^.

126 U. S. GOVERNMENT PRINTING OFFICE : 1964 O - 707-944