National Bureau ot Standards

Library, E-01 Admin. Bids.

NOV 4 1966

NBS TECHNICAL NOTE

408

Superconductive

Materials

and

Some of Their Properties 1

> 0i

: '

:

:

B. W. ROBERTS

4

Q

/'

«.«* OF

%

U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

;
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NBS TECHNICAL NOTE 408

ISSUED SEPTEMBER 26, 1966

Superconductive Materials and

Some of Their Properties

B. W. Roberts

General Electric Research

and Development Center

Schenectady, New York, 12301

A report prepared for the

Office of Standard Reference Data

Institute for Basic Standards

National Bureau of Standards

Washington, D.C., 20234

NBS Technical Notes are designed to supplement the Bureau's regular publications program. They provide a means for making available scientific data that are of transient or limited interest. Technical Notes may be

listed or referred to in the open literature.

For sale by the Superintendent of Documents, U.S. Government Printing Office, Washington, D.C., 20402

Price 45 cents.

Foreword

The National Standard Reference Data System is a government -wide

effort to give to the technical community of the United States optimum access

to the quantitative data of physical science, critically evaluated and compiled

for convenience. This program was estahlishcd in 1963 by the President's Office

of Science and Technology, acting upon the recommendation of the Federal Council

for Science and Technology. The National Bureau of Standards has been assigned

responsibility for administering the effort. The general objective of the System

is to coordinate and integrate existing data evaluation and compilation activities

into a systematic, comprehensive program, supplementing and expanding technical

coverage when necessary, establishing and maintaining standards for the output of

the participating groups, and providing mechanisms for the dissemination of the

output as required.

The NSRDS is conducted as a decentralized operation of nationwide scope with

central coordination by NBS. It comprises a complex of data centers and other

activities, carried on in government agencies, academic institutions, and nongovernmental laboratories. The independent operational status of existing critical

data projects is maintained and encouraged. Data centers that are components of

the NSRDS produce compilations of critically evaluated data, critical reviews of

the state of quantitative knowledge in specialized areas, and computations of useful functions derived from standard reference data.

The primary output of the NSRDS—compilations and critical reviews —is to be

published in a new series, called the National Standard Reference Data Series, within the NBS publications program. However, it has become apparent that uncritical

data compilations which are essential elements of the compilation and evaluation

process, have a substantial value of their own to the technical public. Plans have

therefore been made to publish a number of uncritical data compilations. Some of

these will appear as NBS Technical Notes; others will be published and distributed

through channels connected with their authors or cosponsors.

Ill
Contents

Introduction 1-1

General Properties of Superconductors II-l

High Field Superconductivity III-l

Criteria for the Existence of the Superconductive State IV1

Metallurgical Aspects V-l

Notes Concerning Data in the Monograph VI -1

Properties of Superconductive Elements VII-1

Tabulation of Superconductive Materials VIII-1

High Magnetic Field Superconductive Materials

and Some of their Properties IX-1

Bibliography X-l

Review Articles and Books on Superconductivity.. XI -1

Author Index by Reference Number XI I -

1

IV
Superconductive Materials and Some of Their Properties

B. W. Roberts

This is a noncritical compilation of data on superconductive materials that has been extracted from the

literature published between October 1963 and December 1965.

The properties concerned are composition, critical temperature, critical field crystallographic data, and lowest

temperature tested for superconductivity. The compilation

also includes, bibliography, general reference review

articles and a special tabulation of high magnetic field

superconductors

.

Key Words: Bibliography, compilation of data, composition,

critical field, critical temperature, crystallographic data, low temperature, superconductivity.

INTRODUCTION

This monograph extends the data set on superconductive materials published in Vol. IV of Progress in Cryogenics, 1964, pages 160-231 (subsequently denoted as PC IV) . The new material includes that readily available

to the author subsequent to October 1963 up to approximately December 1965.

The format has been maintained except for several minor modifications such

as an indication of those references which contain data on thermodynamic

parameters, for instance, electronic specific heats and Debye temperatures.

(1-1)
(1-2)

More than one-half century of research on superconductivity

has led to a current steady world activity in attempts at further

understanding and exploitation. The use of superconductive coils

to produce high magnetic fields, now approaching 150 kilogauss,

has spawned a modest business activity for several companies.

A superconductive device called a flux pump has been developed

to energize the superconductive coils to their high current carrying

levels. Extensive studies have been made at all major high energy

particle centers to ascertain the applicability of superconductive

magnets to particle accelerators.

Extensive additional studies on superconductive materials

have been observed in the last three years. In the PC IV article

more than 900 entries were presented. This addendum includes

more than 500 additional entries. Thus the explosion of knowledge

on superconductive materials continues as suggested by extrapolation

in Figure 1 of PC IV.
(II -1)

GENERAL PROPERTIES OF SUPERCONDUCTORS

The historically first observed and most distinctive property

of a superconductive body is the near total loss of resistance at

a critical temperature T characteristic of each material. Figure

1(a) illustrates schematically two types of possible transitions.

The sharp vertical discontinuity is indicative of that found for

a single crystal of a very pure element or one of a few well

annealed alloy compositions. The broad transition, illustrated

by broken lines, suggests the transition shape seen for materials

that are inhomogeneous and contain unusual strain distributions.

Careful testing of the resistivity limits for superconductors shows

-23

that it is less than 4 x 10 ohm-cm, while the lowest resistivity

-13

observed in metals is of the order of 10 ohm-cm. If one compares

the resistivity of a superconductive body to that of copper at

room temperature the superconductive body is at lrast 10 times

less resistive.

The temperature interval AT , over which the transition between

the normal and superconductive states takes place, may be of the

order of as little as 10 K or several degrees in width, depending

upon the material state.

A superconductive body below T , as exemplified by a pure metal,

exhibits perfect diamagnetism and excludes a magnetic field up to

some critical field H , whereupon it reverts to the normal state

as shown in the H-T diagram of Figure 1(b).
(II-2)

The difference in entropy near absolute zero between the

superconductive and normal states relates directly to the electronic

specific heat,y;

<s

s

- Vt-o " VT
(II-3)

(a)

NORMAL

(0

Figure 1. Physical properties of superconductors, (a) Resistivity versus

temperature for a pure and perfect lattice (solid line) . Impure and/or imperfect lattice (dashed line) . (b) Magnetic field- temperature dependence

for Type I or "soft" superconductors, (c) Schematic magnetization curve

for "hard" or Type II superconductors.
(III-l)

HIGH FIELD SUPERCONDUCTIVITY

The discovery of the large current -carrying capability of

Nb-Sn and other similar alloys has led to an extensive study of

the physical properties of these alloys. In brief, a high field

superconductor, or Type II superconductor, passes from the perfect

diamagnetic state at low magnetic fields to a mixed state and

finally to a sheathed state before attaining the normal resistive

state of the metal. The magnetization of a typical high field

superconductor is shown in Figure 1(c). The magnetic field values

separating the four stages are given as H ., H , and H _. The

superconductive state below H is perfectly diamagnetic just as

one obtains for most pure metals of the "soft" or Type I superconductor type. Between H , and H _ a "mixed superconductive state"

cl c2

is found in which fluxons (a minimal unit of magnetic flux) create

lines of normal superconductors in a superconductive matrix. The

volume of the normal state is proportional to -4t/M in the "mixed

state" region. Thus at H „ the fluxon density has become so great

as to drive the interior volume of the superconductive body completely

normal. Between H „ and H the superconductor has a sheath of

current-carrying superconductive material at the body surface, and

above H _ the normal state exists. With several types of careful

measurement, it is possible to determine H ,, H n , and H „. This

cl c2 c3

data set includes those values now presented in the literature for

these high field parameters.
(III-2)

The high field superconductive phenomena are related to

specimen configuration. For instance, the Type I superconductor,

Hg, has entirely different magnetization behavior in high magnetic

fields when contained in the very fine set of filamentary tunnels

in an unprocessed Vycor glass. The great majority of superconductive

materials are Type II. The elements in very pure form with the

possible exceptions of vanadium and niobium and a very few very

stoichiometric and well annealed compounds are Type I.
(IV-1)

CRITERIA FOR THE EXISTENCE OF THE SUPERCONDUCTIVE STATE

Experimental and theoretical attempts to evolve concretely

the criteria for superconductivity in elements, alloys and materials

still persist. A useful criterion has been found in Matthias'

rules. These were developed empirically and then qualitatively

shown to be derivable from the electronic properties of the atoms

as presented in the periodic table. The primary empiricism of

Matthias 1 rules is the prediction that alloys with average numbers

of valence electrons per atom on the low sides of valence 5 and

valence 7 will with some probability have high T . The average

number of valence electrons is taken directly from the periodic

table and an example of the validity of the empiricism is shown

in Figure 2. Here the critical temperature of the known superconductive

compounds having the A15 (/} -W) or CrO~ crystal structure are shown

with the critical temperatures plotted versus the mean number of

valence electrons per atom. Other parameter considerations such

as the atomic volume and the mass of the constituent atoms have

been useful but only in comparison within very similar systems.

Some semiconductive compounds have been found to be superconductive when studied after or during the application of high

pressure. Recently the very high pressure phases of silicon and

germanium have been shown to become superconductive in new dense

phases. The additional discoveries of superconductive modifications
(IV-2)

of antimony and bismuth and the discovery of the very low critical

temperature of tungsten leads to the repeated prediction that all

metals are superconductive even if critical temperatures are currently

too low to be measured. Some valid correlations now suggest that

the noble metals such as gold and platinum will be superconductive

-4 -5 if taken to temperatures of a few times 10 or 10 °K.

The crystal structure of known superconductors has been a

useful guide in discovering others. The classic example is the

large number of superconductive A15 compounds. Other crystal

structures such as the Laves phases and theX-phase or «(-Mn structure

show a pronounced tendency to be superconductive. It is thought

that the crystal structure has a secondary influence on the critical

temperature, however, and that the important consideration is

the electronic structure which leads to a high density of electron

states at the fermi level. Since very few band structures are known

for alloys with the structural complexity of the A15 type, little

general theory has been achieved to date. Correlations of the

electronic specific heat the the Debye 0's have tended to confirm

the BCS (Bardeen-Cooper-Schrieffer) prediction within selected

groups of superconductive materials. However there is evidence

that precise correlation with the BCS theory is not always possible.

One notable change in the data presented are the new very

low critical temperatures and the number of non-superconductive

materials studied down to temperatures well below 1°K. A
(IV- 3)

disappointing and possibly frustrating result is the lack of

discovery of new superconductive materials with critical temperatures

greater than 18.5°K. This outlines a definite theoretical problem.

Is there a limit to superconductive critical temperatures somewhere

in the vicinity of 19 or 20 K or are there undiscovered materials

with critical temperatures above this? The technical desirability

of finding superconductors with higher T follows since critical

magnetic fields will be proportionately higher.
15

To'o

-SUPERCONDUCTIVE

TRANSITION TEMPERATURE.

?-N0T SUPERCONDUCTIVE

TO THIS TEMPERATURE

4.7

Kl

• •

/I

• %

6.5

/

/

r- r

* v • • \

3 4 5 6 7

VALENCE ELECTRONS /ATOM

(IV-4)

Figure 2. Critical temperature versus valence

electron/atom ratio for '^-W or A15 (Cr,0)-

type compounds.
(v-i)

METALLURGICAL ASPECTS

The sensitivity of superconductive properties to the material

state is most pronounced and has been used in a reverse sense to

study and specify the detailed state of alloys. The mechanical

state, the homogeneity, and the presence of impurity atoms and

other electron scattering centers are all capable of controlling

the critical temperature and the current -carrying capabilities

in high magnetic fields. Well annealed specimens tend to show

sharper transitions than those that are strained or inhomogeneous.

This sensitivity to mechanical state underlines a general problem

in the tabulation of properties for superconductive materials.

The occasional divergent values of the critical temperature and

of the critical fields quoted for a Type II superconductor may

lie in the variation in sample preparation. Critical temperatures

of materials studied early in the history of superconductivity

must be evaluated in light of the probable metallurgical state

of the material as well as the availability of less pure starting

elements. It has been noted that recent work has given extended

consideration to the metallurgical aspects of sample preparation.
(VI -1)

NOTES CONCERNING DATA IN THE MONOGRAPH

Table 1 lists the elements and some of their superconductive

properties. The data have been selected generally from recent

studies in which sample purity and perfection appear to have been

considered. The data given have not been critically evaluated.

Table 2 contains superconductive materials reported during

the period plus all materials that have been reported to be tested

specifically for a superconducting transition down to some temperature T without discovery of a transition. All compositions are

denoted on an atomic basis, i.e. AB, AB or AB for compounds,

unless noted. Solid solutions or odd compositions may be denoted

as A B n , or A B. A series of three or more alloys is indicated

z 1-z z as A B or by actual indication of the atomic fraction range such

x y as A_ _ ,B. _ , . The critical temperature of such a series of 0-0.6 1-0.4

alloys is denoted by a range of values or possibly the maximum

value. In many cases several references will be found for the

same alloy. This usually denotes a separate measurement by each

source, and in a few cases may even indicate a disagreement over

the superconductive properties. In view of the previous discussions

concerning the variability of the superconductive properties as

a function of purity and other metallurgical aspects, it is

recommended that the appropriate literature be checked to determine

the most probable critical temperature or critical field of a

given alloy. Another unfortunate point lies in the selection of
(VI -2)

a number for the critical temperature from a transition observed

in the effective permeability or the change in resistance, or

possibly the incremental changes observed in frequency observed

by certain techniques. Most authors choose the mid-point of

such curves as the probable critical temperature of the idealized

material, and others will choose the highest temperature at which

a deviation from the normal state property is observed.

Table 3 lists a supplementary tabulation of high magnetic

field superconductors.

A list of review articles primarily concerned with the

experimental and material aspects of superconductivity is appended

as well as a complete alphabetical cross-reference to authors by

reference number.

Acknowledgements

Preprints and courtesy copies of reports on superconductive

materials have been kindly sent by many researchers in the field

and found most useful and are gratefully acknowledged. Skilled,

persistent and dedicated assistance of Mrs. Marilyn Brown and

formerly of Mrs. Jean Slaggie have greatly contributed to the

accuracy and completeness of this monograph. The thorough coverage

of the scientific literature is due to the library staff's fine

efforts in seeking pertinent articles, especially by Mrs. Ethel

Fontanella and Mrs. Maryde Orr.
(VII-1)

Table 1. Properties of Superconductive Elements (References given in Table 2, as well as Crystal

Structure Data and Information on Non-superconductive Elements)

T

c (°K) H I [oersteds)

© D

(°K) (mJ

y

-1 -2 Element Cal. Mag. Cal. Mag. mole deg.K )

Al 1.183 1.196 104 99 420t 1.36 ft

Cd 0.54, 0.,518 0.56 29. 6 30 209 0.688

Ga 1.087, : L.078 1.091 59. 4, 58 .9 51 317, 324.7 0.601, 0.596

Kg (4) 4.16 4.153 380 412 87, 71.9 1.91, 1.79

Hg Os) 3.949 339 93 1.37

In 3.396 3.40 35 278 293 109 1.81

Ir 0.14 19 3.1

La (o|) 4.80 -5.0

La (tf) 5.91 6.06 1,600 132 6.7

Mo 0.915-0,,918 0.92 95 98 382-461, 470 1.81-1.89, 1.9:

Nb 9.17 9.22, 9. 47 1,944 1,980, HF* 238, 271 7.53

Os 0.655 65 2.35

Pa 1.4

Pb 7.23 7.193 803 96.3 3.0 Re 1.699 1.698 188 198 210 2.35

Ru 0.49 66 2.4

Sb 2.6-2.7 HF*

Sn 3.722 3.722 303 309 195 1.75

Ta 4.39 4.483 780 830, HF* 255 6.4

Tc 8.22

Th 1.368 131 162 168 4.65

Ti 0.42 0.39 56 100 430, 415 3.30

Tl 2.38 2.39 176.5 171 78.5 1.47

U («() 0.68 206 10.6

U (pseudo-y) 1.80 (extra po la ted va'.Lue)

V 5.03 5.30 1 ,310 1,020, HF* 338 6.4

w 0.012 1,070

Zn 0.852 0.875 51.8 53 309 0.66

Zr 0.546 47 265 2.9

Zr (co) 0.65
(VII -2)

Element

T

c <°K) H (oersteds)

o Cal. Mag. Cal. Mag. (°K> (mJ mole" 1 deg.K

-2

)

Thin films formed below 10 K

Be

Bi

Ga

In

Sn

~6, -8.4

-6.0

8.4

3.95-4.25

4.6-4.7

H „»11

cz

Under high pressure

Bi II

Bi III

Ge

Se II

Si

Te

3.916

3.90 3.86

7.25

4.85-5.4

6.75, 6.95

7.1

~3.3

Pressure

25,000 atm

25,200 atm

26,800 atm

27,000-28,400 atm, HF*

-120 kbar

-130 kbar

Pressure

120-130 kbar — 56,000 atm

f For another data set see Mendelssohn, K. , Cryophysics, p. 178 (Interscience, New York, 1960).

t Parkinson, D. H. , Rep. progr. Phys. 21, 226 (1958)..

See later table for additional data onH ., H „ and H „. cl' c2 c3
(VIII -1)

Table 2. Tabulation of Superconductive Materials (including Proven

Non-superconductors) with Critical Temperatures and Fields, Some

Crystal Structure Data, and References

Symbol s used:

* Eutectic alloy.

A Uncertain composition.

R Resistance measurements.

M Denotes maximum T in specimen series.

c ** T is the lowest temperature at which a material has been

n

checked for a superconductive transition.

HF In H column indicates that some information is available in

o Table 3 on high field magnetic properties.

V On material or reference indicates a thin film study.

o° All cell edges are intended to be quoted in Angstrom units.

T' ( ) Denotes incremental changes in T from pure metal.

o Impure material.

C Calorimetric determination.

VA Valence electron/atom.

SS Solid solution.

n Number of carriers in semiconductive materials.

# Electronic specific he.t Debye data given.

(Some of the above symbols may be found only in PROGRESS IN CRYOGENICS

article.)
(VIII-2)

Key to Crystal Structure Types Found in Table 2

"Struckturbericht"

Type* Example Class

Al Cu Cubic, f.c.

A2 W Cubic, b.c.

A3 Mg Hexagonal, close packed

A4 Diamond Cubic, f.c.

A5 White Sn Tetragonal, b.c.

A6 In Tetragonal, b.c.

(f.c. cell usually used'

A7 As Rhombohedra

1

A8 Se Trigonal

A 10 Hg Rhombohedra

1

A 12 oj-Mn Cubic, b.c.

A13 >S-Mn Cubic

A15 >0-W Cubic

Bl NaCl Cubic, f.c

B2 CsCl Cubic

K8

1

NiAs Hexagonal

B8

2

Ni

2

In Hexagonal

BIO PbO Tetragonal

Bll r-CuTi Tetragonal

B17 PtS Tetragonal

B18- CuS Hexagonal

* See W. B. Pearson, Reference 108, p. 79
(VIII -3)

"Struckturbericht"

Type* Example Class

B20 FeSi Cubic

B27 FeB Ortho -rhombic

B31 MnP Ortho -rhombic

B32 NaTl Cubic, f.c.

B34 PdS Tetragonal

B

f

S-CrB Ortho -rhombic

B

g

MoB Tetragonal, b.c.

Bh

WC Hexagonal

B.

X

r'-MoC Hexagonal

CI CaF

2

Cubic, f.c.

C1

b MgAgAs Cubic, f.c.

C2 FeS

2

Cubic

C6 Cdl

2 Trigonal

Cllb MoSi

2 Tetragonal, b.c.

C12 CaSi„ Rhombohedral

C14 MgZn

2

Hexagonal

C15 Cu

2

Mg Cubic, f.c.

C15ub

AuBe Cubic

C16 CuAl

2

Tetragonal, b.c.

C18 FeS, Or tho -rhombic

C22 Fe

2

P Trigonal

C32 A1B„ Hexagonal
(VIII -4)

"Struckturbericht"

Type* Example Class

C36 MgNi

2

Hexagonal

C37 Co

2

Si Or tho - rhomb ic

C49 ZrSi

2

Ortho -rhombic

C54 TiSi

2

Ortho -rhombic

C

c Si

2

Th Tetragonal, b.c.

do

3

BiF

3 Cubic, f.c.

DO uFe

3

C Ortho -rhombic

D0

18 Na^As Hexagonal

D0

19

Ni Sn Hexagonal

D020 NiAl

3

Ortho -rhombic

D0

22 TiAl

3 Tetragonal

DO

e Ni

3

P Tetragonal, b.c.

DI3 Al.Ba

4 Tetragonal, b.c.

Dl

c PtSn.

4

Ortho -rhombic

D2

c MnU.

6 Tetragonal, b.c.

D2,

a CaZn Hexagonal

D5

2 ^2°3 Trigonal

D5

8

Sb

2

S

3

Ortho -rhombic

D7

3 Th

3

P

4 Cubic, b.c.

D7

b

Ta

3

B

4 Ortho -rhombic

D8, Fe

3

ZnW

Cubic, b.c.

D8

2 Cu

5

Zn

g

Cubic, b.c.
(VIII-5)

"Struckturbericht"

Type* Example Class

D83 CU

9

A1

4

Cubic

D8g Mn

5

Si

3 Hexagonal

D8

b

CrFe Tetragonal

D8.

1

Mo

2

B

5

Rhombohedral

D10

2

Fe

3

Th

7

Hexagonal

E9

3

Fe

3

W

3

C Cubic, f.c.

L1 CuAu Tetragonal

Ll

2

Cu Au Cubic

L

2b

ThH

2 Tetragonal, b.c.

L

3

Fe

£

N Hexagonal
(VIII -6)

Material T

c (°K) H (oersteds) T ** Crystal structure co o n

Ref.

Ag

3 _ 3Al

Ag

5Ba

Ag

0. 95-0. 81

Ga

0. 05-0. 19 Ag

0. 80-0. 30Ga0. 20-0. 70 Ag

0. 29-0. 02

Ga

0. 71-0. 98 Ag Ga Inn lri °x y . 10 Ag Ga Sn °x y . 10 Ag Ga Znn °x y 0.10

Ag

4Ge

Ag

0.438Hs0.562

22.

AgjSr

AgTe,

Al Au

ALAu,

Al

2CCr

3

Al

2CMo

3 AlCNb„

Al

2CNb

3

Al

2CTa.

A1

2CTi

3

A1

2CV

3

Al Co Fp

0.107 0.088 0.805

A1

0.107Co 0.176Fe

0.717 A1

0.107Co 0.259Fe0.634

6.5-8

6.5-8

4.2

6.5-8

0.85

0.64

Ag

3In

Ag

Q jTn

gTe (n=1.40xlo") 1.20-1.89

Ag

Q 2In

Q gTe (n=l. 07xl022

) 0.77-1.00

AsSi„

Ag

5 Sn

2.6

0.4-0.7

10.0

0.34 like A13, a=6.92

0.34 D2

d

, a=5.71, c=4.64

1.4

1.4

1.4

1.4

Hex. , h.c. p.

D8-, ? 3 "gainma brass,'

complex, b.c.c.

Bl, a=6.12

Bl, a=6.08

0.34 A3, a=2.94, c=4.77

0.34 D2,, a=5.68, c=4.62

a Cubic, primitive

0.34 CI, a=6.01

Like A13, a=6.92

4.2 Hex., "H-phase,"

a=2.47, c=7.39

A13, a=6.867

4.2 Hex.

4.2 Hex. , "H-phase,"

a=2.67, c=8.02

4.2 Hex. , "H-phase,

a=2.68, c=7.97

4.2 Hex. , "H-phase,"

a=2.63, c=7.87

4.2 Hex. , "H-phase,

a=2.52, c=7.52

1.4 Cubic

1.4 Cubic

1.4 Cubic

486

486

533

533

533

5 33

533

533

487

489, 511

533

470

470

533

486

486

487

486

486

496, 497

496, 497

497

496, 497

496, 497

496, 497

496, 497

514#

514#

514#
(VIII -7)

Material T

c

(°K) H (oersteds) T ** Crystal Structure co Ref.

A10.118

C °0.446Fe0.436

Al Co Fp

0.118 0.523 0.359

Al fn Ve* 0.119 0.352 0.529

A1

0.119

C°0.610Fe0.271

A1

0.049

Cr0.951

A10.10

Cr0.90

A10.146Cr0.854

A1

0.20

Cr0.80

Al Cr 0.250^ 0.750

si p r 0.30 0.70

A1

0.089Cr0.544Fe0.367

Al Cr Fp

0.09 0.046 0.866

Al Cr Fp

0.09 0.228 0.682

A10.091Cr0.817Fe0.092

A1

0.095

Cr

0.45 3Fe

0.452

A10.096Cr0.679Fe0.225

AT Cr Vp

0.097 0.726 0.177

A10.100Cr 0.632Fe0.268

AT Cr To 0.104 0.849 0.047

A10.105Cr0.75 3Fe

0.142

A1

0.10Cr0.63 V

0.27

A10.111Cr0.801V

0.089

A10.114Cr0.267V 0.618

A1

0.115Cr0.708V

0.177

A1

0.115Cr0.839V

0.045

A1

0.122Cr0.458V

0.42

AT Cr V

0.131 0.088 0.781

Al

2La

A1

0. 19-0. 30Nb

0. 81-0. 70

1.46

3.2

17. 3M

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 A2

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

1.4 Cubic

Cubic

C15, a=813

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

514#

486

479

(As cast)

A1

0. 19-0. 30Nb

0. 81-0. 70 (Annealed)

18. 3M 479

Al Nb n X 1-K Al Nb, X 1-x6-9

<4.2-13.5

Cubic 497

D8, , 3=9.318, c=4.813 497

to a=9.295, c=4.819
(VIII -8)

Material

Al Nbx 1-x Al Nb,

x 1-x Al Nb., x 1-x AlNb„

A10.27

Nb 0.73

A1

0.27

Nb

0.7 3-0.48V

0-0.25

A1

0.27Nb 0-0.50V0.73-0.23

AINb V

x y AlPbV (superimposed films)

AlPt

Al

2 Pt

A1

0.10Tx0.63

V

0.27

A10.11TX 0.149V0.741

A

1

T-i V

0.120 0.328 0.552

A1

0.125Tl0.520V0.355

A1

0.127T:L 0.693V0.130

A

1

Ti V

0.15 0.595 0.255

A

1

Ti V

0.25 0.525 0.255

A10.30

T:L 0.49V

0.21

ATL V

0. 108 0.892

AT V 0.188 0.812

Al V

0.27 0.73

Al V

0.308 0.692

AT V

0.402 0.598

A1

2Y

T

c (°K) H (oersteds)

12-17.5

12

17.5

12.5-17.5

17.5

14.5-17.5

T ** Crystal Structure o> n

J Ref.

<4. 2-13.5

1.2-7

0.48-0.55

3.62

2.05

2.70

3.44

3.52

2.36

1.82

^22, As„ ,,InTe. ,, (n=l. 24x10 ) 0.85-1.15

0.33 0.67 '

As

Q 5 InTe

Q (n=0. 97xl0 22

) 0.44-0.62

Aslr

Aslr

AsPd„ (low temperature)

AsPd„ (high temperature)

As?d„ (quenched)

AsPd„ (annealed)

AsPd.

0.60

1.70

1.71

0.6

4.2

A 15

A 15, a=5.196

A15, a=5.185

A 15

A15, a=5.185

A15, a=5.136-5.185

Cubic, a=3. 055-3. 18

0.34 Cubic, a=4.85

CI, a=5.92

Cubic

Cubic

Cubic

Cubic

Cubic

Cubic

1.4 Cubic

1.4 Cubic

Cubic

1.4 Cubic

4.2 Cubic, a=3.055

1.4 Cubic

1.4 Cubic

0.34 C15, a=7.86

Bl, a=5.98

31, a=5.91

0.35

0.35

Hex. , a=9.79, c=6.62

C22, a=6.65, c=3.58

C22, a=6.65, c=3.57

Hex. , a=9.79, c=6.61

0.35 DO , a=9.986, c=4.830

e'

513

513

513

497

497

497

497

497 512V

486

486

514#

514#

514#

514#

514#

5I4#

514#

514#

514#

514#

497

514#

514#

486

470

470

491

491

491

491

530

530

491
(VIII -9)

Material T

c <°K) H (oersteds) T ** Crystal Structure co o n

J Ref.

AsPd.

AsPd.

As

2Pd

As

2Pd

5 As

2Pd

As

2Pt

As

3Pt

2 AsRh

AsRh1.4-1.6

AsRh

1.4

AsRhn , 1. 6 AsRh,

7 (quenched)

AsRu

AsRu

2 AsSn (n=2. 14x10"

As^2Sn-3

,22,

,22, As-Sn, (n=0. 56x10 ) Au (rapid quench)

Au Ba

Au^Ca

AuGa

AuGa,

Au

0.30Ge0.70 Au 0.33Ge

0.67 Au

0.40Ge0.60 Au0.47Ge0.53

Au0.50Ge0.50 Au0.54Ge0.46 Au

0.61Ge

0.39 Au

0.70Ge0.30 Au

0.725

Ge0.275

Au

0.75Ge0.25 Au

0.775

Ge

0.225

0.46

0.43-0.50

0.58

<0. 03-0. 56

3.41-3.65

3.5-3.6 , 1.21-1.17

1.16-1.19

0.4-0.7

0.34-0.38

1.2

1.63

1.63

1.63

1.50

1.31

1.09

0.99

Trace @ 0.5

Trace @ 0.5

0. 3 DO , a=9.98, c=4.83

e 530

1. 1 5 30

1. 1

Complex

530

491

5 30

0. 35 491

0. 35 491

B31, a=5.65, b=3.58, c=6. 00 491

Hex. 491

Hex., a=9.15, c=3.53 491

+ weak a=9.15, c=5.19

Hex. , a=9.32, c=3. 67 491

Ortho. Rh.As + Rh- ,As

, 2 1.6 phase

491

0. 35 491

0. 35

Bl, a=5.72

Rhomb., a=12.23, *=19.2 3

491

470

470

470

.32 Al, f.c.c.

D2

d

, a=5.69, c=4.54

C15, , a=7.747

D

487

486

486, 5 35

B31, a=6.40, b=6.27, c=3 .42 486

.34 CI, a=6.07 486

.32 h. c. p. + Ge 487

.32 weak complex + h.c.p. + Ge 487

h.c.p. + Ge + weak compli5X 487

complex + weak Ge 487

complex + weak Ge 487

complex 487

complex 487

complex 487

complex + weak h.c.p. 487

.32 Hex., h.c.p. + weak complex 487

.32 Hex., h.c.p. weak + comp!Lex 487 + f.c.c.
(VIII -10)

Material T ( K) H (oersteds) T ** Crystal Structure Ref.

Au

0.90Ge0.10 Au

0.92

Ge

0.08 Au

0.80Hg

0..20 Au 0.85Hs

0..15 Auln

Auln~

Au

5K

Au„Na

AuNb.

Au

0.02

Kb

3Rh

0.98

^0.05^3^0.95

Au

0.10

Nb

3Rh0.90 Au

0.30

Nb

3Rh0.70

Au

0.50Nb

3Rh0.50

Au

0.70

?Tb 3Rh

0.30

Au

0.90Nb

3Rh

0.10 Au

0.95Nb

3Rh0.05 Au

0. 98^3^0. 02 AuPb„

AuPb V

AuPb

AuPb

3V

Au ?b

Au

5Rb

AuSn

Au Sn

Au

3Te

5 AuTi„

BCMo,

B C. Mo (quenched)

x 1-x n ' BMo

BTi

B

2Ti

BW„

Trace (3 0.9

Trace @ 0.9

0.4-0.6

11.5

2.53

2.52

2.70

4.6

6.6

9.5

10.8

11.0

10.9

3.15

4.3

4.40

4.25

1.18

1.25

0.7-1.1

1.62

5.4

14.2

(broad 17.5-12.2)

0.5 (extrapolated)

0.32 Cubic, f.c.c.

0.32 Cubic, f.c.c.

0.32

0.32

Complex

0.34 CI, a = 5.51

0.34 D2., a=5.64, c=4.4E

d' ' 0.34 C15, a=7.8i

A15, a=5.2027

A15, a=5.133

A15, a=5.137

A15, a=5.1412

A15, a=5.1573

A15, a=5.1688

A15, a=5.1827

A15, a=5.1960

A15, a=5.200

A15, a=5.203

C15, a=7.94

0.34 D2,,a=5.6, c=4.4

d B8

1

, a=4.32, c=5.52

A3, a=2.92, c=4.77

Primitive cubic

A15, a=5.094

Ortho -rhombic

Cubic + some Hex.

B27, a=6.12, b=3.06, c

C32, a=3.030, c=3.227

3.1

487

487

489

489

486

486

486

486

492

492

492

492

492

492

492

492

492

492

475, 521

521"

475, 521 521^

486

486

486

486

487

522

497

497

497

=4.56 522

522

474
(VIII -11)

Material T

c (°K) H (oersteds) T ** Crystal Structure cr> o

v n

J Ref.

Be^

Bill

Billl

Bi 0.019

In0.981

Bilr

Bilr

£ BiNb_

BiNb~ (high pressure

and temperature)

Bi

i-opbo-iv

Bl

0.95

Pb 0.05^

Bi Ph ^

0.99 0.01

C 1&Rb (blue)

CTa V7 (sputtered)

CTa

2 CTi

CaCu,.

CaZn,.

Cd

Cd (isotopes)

6.5

3.86

3.05

7.25-8.67

BiRu

BiRu„

C (pyrolytic graphii:e)

CgCs (gold) 0.020-0.135

C 16Cs (blue)

C

gK (gold) up to 0.55

C 16K (blue)

°IC, Mo (quenched) 14.2

C, Mo (quenched) 8.8

C. Mo (quenched) 9.4-11.7

C 0.40Mo

0.60 (quenched) 11.7

CM°0.83Ti

0.17 10.2

CNb

2 9.1

C~0.7- 1.0^0. 3-~0 6-11

C„Rb (gold) 0.023-0.151

5.09

3.2

0.518

HF

HF

HF

HF

29.6, HF

0.35

0.35

2.25 Cubic, a=3. 327

A15, a=5.320

1.03

1.03

0.35

0.35

0.011

0.011

0.011

Cubic + some Hex.

Hex. , v^ Mo,C„

r>Mo,C '32 + partial** r MoC, 497 1-x

550^

437

437

544

491

491

508

508

484^

484^

484"^

491

491

494

494

494

494

494

497

497

Some Bl

Bl, a=4.290

Bl

0.011

Bl, a=4.329

0.34 D2

d

, a=5.09, c=4.09

0.34 D2 , a=5.42, c=4.19

497

522

474

497

494

494

5057

474

522

486

486

537

546
(VIII -12)

Material T

c (°K) H (oersteds)o T ** Crystal Structure x> n

Ref

.

Ce (0-10,000 atm.)

Celr

3 Celr

5 Celr, „

3.34

1.82

CePt

2 CePt.

CePt,

Ce

0. 20-0. 173

Pt

0. 80-0. 826

CoLa,

CoLu„

Co„Lu

Co 0.02Nb

3Rh0.98

Co 0.05Nb

3Rh0.95

Co 0.10Nb

3Rh0.90

CoSc„

CoSc.

Co

0. 28-0. 32Sc

0. 72-0. 68

Co Th

Co Ti

x y

C °0.28Y

0.72

CoY„

CoY

CrCr^

Ct Ti 0.025 0.975

Cr Ti (quenched)

x y

M ' Cr Ti

x y Cr0.011

Tl

0.967

V0.022

Cs

CS 0.32°3W

Cu

Cu.Ga

CuTi

1.26-0.70, 1.55M

(portion only)

4.01

0.35 +++

(portion only)

2.28

1.96

1.90

0.35

(portion only)

0.34

0.34^T (portion only)

3.5

3.6

1.12

1.25 "(-Ce dense f.c.c.

0.32 C15, a=7.581

0.32 C15, a=7.730

0.32 C15, a=7.640

0.32 D2

d

, a=5.369, c=4. 385

DO a=7.279, b=10.088,

ZU c=6.578

0.32 C15, a=7.123

A15, a=5.132

A15, a=5.135

A 15, a=5.1347

0.32 C16, a=6.374, c=5.616

0.32

0.32 D2., a=5.005, c=3.987

d

0.32

1.4 A2

0.3

1.1

Fe PPd

0.5 3 +++ Beginning of transition

0.011

1.4

0.35

-CO?

Hex. , a=7.4, c=7.i

Bll, a=3.108, c=5.887

542

469

469

469

469

469

469

469

469

469

469

492

492

492

469

469

469

469

522

469

469

469

514#

503V

477 #

523

522

477 #

494

500

537#

533

522 491
(VIII -13)

Material T

c

(°K) H

q (oersteds) T ** Crystal Structure en Ref.

Fe Ti

0.01 0.99

Fe Ti

0.015 0.985

Fe Ti

0.08 0.92 Fe Ti

x y

2.3

2.8

Ga 1.078

GaN

GaPt

Ga

2Pt 1.7-1.9

0.23-0.26 0.77-0.74 14. 3M (annealed)

Ga

0. 23-0. 26V

0. 77-0. 74

14. 5R

(annea led) Ge ("120 kbar pressure) 4.85-5.4

Ge

? lr3 0.87

(portion only) GeMo

3 1.4

GeNb_ (quenched) 17.-6. + some below 4. Ge

0. 25-0. 29^0. 75-0. 71 6.

Ge n oq^h 7! 6.

GePd.

Ge

1.5 Pd

Ge

2Pd

5 GeTe (Ag doped) (n=27xl020

) 20 GeTe (Ag doped) (n=64xl0 ) 20 Gen Te (n=9-16xl0 ) 1-x x

' Ge

0>937

Te (n=14. 3xl0^u

)

7ft Ge

_ 95QTe (n=ll. 8xlO^U

)

7ft Ge0.963Te (n=9 -3xlO zu

) Ge

Q _ 976

Te (n=8.5xl0^ U

) ?o Ge 1.006Te (n=7 - 5xl° ) Ge

3Te4

(n=l. 06xl0 22

)

Ge

2Ti

Trace

0.21

0.41

0.07-0.31

0.30

0.24

0.17

0.07

1.55-1.80

Ge

3Ti

5 GeV„

H

1 -La (with free La)

H 1.96^

6.0

58.9

0.35

0.35

0.02

1.1

0.33

A2

0.34 B20, a=4.91

477 #

477 #

47 7 #

522

537#

528

486

486

479

479

540

491

474

A 15 498

A15 498

A 15, a=5.149 498

491

491

491

481

481

Bl 482

501

501

501

501

501

Rhomb., a=13. 11, <* =17.93 470

C54, a=8.594, b=5.030, 522 c=8.864

D8

8

, a=7.552, c=5.234 522

474

488

488
(VI II -14)

Material T

c (°K) H (oersteds) T ** Crystal Structure m o

v n

J Ref.

H2.03^

H 2.11^

H2.15^

"2.36^

Hg

Hs0.80

Pt0.20

In"

InNbInNb_ (high pressure and

temperature)

In l-0.90

Pb O-0.10

InPd

InRh

InSb

InSb (metallic)

InSbll (quenched)

InSbII 7

J-Sn0>02 _0#80

(quenched)

msbii-/-sn005_080

(heat treated, quenched)

InSbII^.Sn

0>05 _ 0>90

(heat treated, quenched) In

Q 82Te (n=0.83xl0~ 22

In

Q Te (n=0. 88x10

In

Q g? Te (n=1.09zl0

In Te (n=l. 28x10

In

Q g5 Te (n=l. 47x10

InTe (n=1.71xl0

-22

) InTe (n=1.71xl0

-22

) InTe

22

22

22

22

In 1.015Te (n=1.67xl0~ 22

) In

L Q5Te (n=1.58xl0~ 22

) In

x 1QTe (n=1.45xl0" 22

) -22,

4.16

In

2Te

3 22 In.Te, (n=0. 47x10 )

4-8

0.7-1.1

0.7

2.1

1.6-2.1

2.1

4.0-4.4

3.8-4.6

3.8-5.1

1.02-1.06

1.09-1.15

1.40-1.55

1.87-2.04

2.5-2.7

3.2-3.45

3.20-3.45

3.25-3.51

2.95-3.41

2.55-2.80

2.35-2.60

1.15-1.25

380

HF

1100

1.1

1.1

1.1

1.1

0.32

2.25 Cubic, a=3.32(

A15, a=5.303

B2

0.32 B2

/?-Sn structure', a=5.72,

b=3.18

Tet. , a=5.79, c=3.15

1.6

1.0

Bl, a=6.052

Bl, a=6.055

Bl, a=6.081

Bl, a=6.110

Bl, a=6.14

Bl, a=6.16

Bl, a=6.177

InTe (I)

Bl, a=6.178

Bl, a=6.181

Bl, a=6.182

Bl, a=6.179

Rhomb., a=13.75, °<=17.80

488

488

488

488

527#

489

532V

508

508

480#

489

489

471

502

5 39

5 39

539

5 39

506, 515

506, 515

506, 515

506, 515

506, 515

506

470, 515

507

515

515

515

515

515

470, 515
(VI I I -15)

Material T

c CK) H (oersteds) T ** Crystal Structure Co o n

J Ref.

In 1.000Te

l..00211

Ir v

Ir

2La

Ir

3La

Ir

3La? Ir

5 La

IrLu

IrLu„

IrLu,

Ir„Lu

Ir„Lu

Ir

3Lu7 IrNb

Ir

0.02

Nb

3Rh0.98

^0.05^3^0.95

Ir

0. 10^3^0. 90 ^o.so^s^o.yo

Ir0-50Nb

3Rh0>50

Ir0.70Nb

3Rh0.30

Ir

0.90Nb

3Rh

0. 10 IrP

Ir

2P

IrS

IrS 2.6 IrSb

Ir

2Sb

IrSc

0.32 0.68

IrSc.

Ir

2Sc

Ir

2.5

Sc

Ir

2 5 Sc

Ir„

5 Sc

3.5-3.7

0.48"1"1

2.46

2.24

2.13

0.84

(portion only)

2.47

2.89

0.78

(portion only)

2.43

2.38

2.07

2.46

0.42+ (portion only)

2.13++

HF

0.3

0.32

1.7

51, a=6.154

C15, a=7.686

D10

2

, 3=10.235, c=6.473

0.32 B2, a=3.330

C15, a=7.443

C15, a=7.434

A15, a=5.1356

A15, a=5.131

A15, a=5.132

A15, a=5.1329

A15, a=5.1340

A15, a=5.1349

A15, a=5.1349

A 15, a=5.1345

1.7

1.7

1.7

1.7

1.7

0.35

0.35

0.32

0.32

0.35

0.35

0.32 B2, a=3.205

0.32

0.32

C15, a=7.347

C15, a=7.343

507 503^

469

469

469

469

469

469

469

469

469

469

492

492

492

492

492

492

492

492

491

491

552

552

491

491

469

469

469

469

469

469

469

+ Beginning of transition of powdered sample

++ Powder transition
(VIII -16)

Material T (°K) H (oersteds)

o T ** Crystal Structure m n

J Ref.

Ir

3Sc

IrSe,

IrSe

2.9 IrSn

2 Ir 0.5 Te

0.5 IrTe„

IrTe.

IrTh

Ir

3Th

Ir

5 Th

IrV„

Ir V 0.33 2.67

IrY,

Ir Y 0.01 0.99

Ir 0.0175

Y

0.9825

Ir Y

0.65 0.35

Ir Y

0.69 0.31

Ir Y

0.69 0.31

Ir Y

0.70 0.30

Ir

2Y

Ir

2Y

Ir Y

2 3 Ir„ . Y

3 or 4

0.27-0. 31°3W

K0.40-0.57°3W

/?-La

LaPdg

LaPt„

La 0.28Pt0.72

0.65-0.78

3.0+++

1.18

0.37+

4.71

3.93

1.39

0.35

(portion only)

0.49+++

(portion only)

1.38

1.98

1.44++

2.16++

1.09

2.18, 0.88

1.61

3.50

0.50

1.5

6.06

0.46

0.54

0.32

0.32 Ortho-rhombic, a=20.94,

b=5.93, c=3.74

0.32

CI, a=6.34

0.32 C6, a=3.930, c=5.393

C2, a=6.413

B

f

, 3=3.894, b=11.13,

c=4.266

D2,, 3=5.315, c=4.288

a 0.35 A15

A 15

0.32

C15, a=7.525

C15, 3=7.501

C15, a=7.501

C15, a=7.501-7.512

C15, a=7.518

C15, a=7. 500-7. 520

0.011

Hex., a=7.4, c=7.6

Tet. , a=12. 3, c=3.8

Al, a=5.29 (95% Al)

0.32 Ll

2

, a=4.233

C15, 3=7.776

C15, a=7.722

469

552

552

486

552

552

552

469

469

469

498

498

469

469

469

469

469

469

469

469

469

469

469

494

500

500

536

469

469

469

+ Beginning of transition

++ Powder transition

+++ Beginning of transition

of powdered sample
(VIII -IV)

Material T (°K) H (oersted)

o T ** Crystal Structure »n

Ref.

LaPt c

LaRhLaRh.

LaRh E La-Rh,

2.60

1.62

2.58

La.S, + additional compositions 6.5

LaSe

La

2Se

3 La,Se. +additional compositions 8.6

LuRh

LuRh„

Lu 0.275

Rh

0.725

LuRtv

Lu„Rh

Lu

3Rh

Mn0.0028T3"0.9972 (quenched)

Mn

0. 0028-0. 04

Tl

0. 9972-0. 96 (quenched from 1000°C) Mn Ti

0.0028-0.04 0.9972-0.96

(quenched from 690 C) Mnm Ti

0.01 x0.99 Mn

0. 01-0. 14Tl

0. 99-0. 8§ (quenched from 1000 C) Mn

0.02

Ti

0.98 Mn

0.02

T:L 0.98

(quenched)

^O-O.OOSS^y

Mn Ti

x y Mn Ti

x y Mo

Mo 7

Mo

3Si

Mo-Sn

1.27

0.49

2.6R

-3. OR

1.2 <1.4

1.7

1.9

0.2-0.4

0.915-0.918

~5

1.3

HF

HF

95

0.32 D2

d

, a=5.386, c=4.37(

0.32 C15, a=7.646

D10

2

, a=10.145, c=6.434

D7

3

, a=8.73

1. 25

1. 25

D7 3> a=9.05

0. 32 B2, a=3.334

0. 32 C15, a=7.404

C15, a=7.355

0.32

0.32

1.1

0.06

pure =f + pure /?

Mo_Sn (high pressure

and temperature)

A2 + extra lines

1.0 Cubic, a=3.165

0.35 A15, a=5.094

469

469

469

469

469

5 34

5 34

534

5 34

469

469

469

469

469

469

523

523

523

490

523

477

523

490

490

522

54 3#

503^

474

509

509
(VIII -I'd)

Material T (°K) H (oersteds)

o X ** Crystal Structure <» n

Ref.

%.025Ti0.975 Mo0.04Ti0.96 Mo Ti

x y NNb

x NNbV (sputtered)

NNb

x y N Nb Zr

x y z NTaV (sputtered)

NTa ^ (sputtered)

Na 0.2°3W

Na 0.23-0.35°3W

Na 0.10°3W

Na O.W

x 3 Nb

Nb

Nb v

Nb v (2000-20000$)

NbV (420-6000$)

Nb?

NbO

Nb-Os

Nb

3Os 0.02

Rh

0.98

Nb 3° S 0.05

Rh

0.95 Nb 3° S 0.10

Rh 0.90

Nb 3° S 0.30

Rh

0.70

Nb 3° S 0.50

Rh0.50

Nb 3° S 0.70

Rh 0.30

Nb 3° S 0.90

Rh0.10

Nb

3Pd0.02Rh0.98

Nb

3Pd0.05

Rh 0.95

Nb

3Pd 0.10

Rh0.90

Nb Pt

Nb

3PC0.02

Rh0.98

Nb

3Pt 0.05Rh

0.95

1.8

2.0

6-9

13.5-17.0

4.84

0.55

0.56

9.22 + 9.25*

6.5-9.4

6.70-9.11

<bulk

1.25

2.42

2.39

2.30

* Residual Resistivity Ratio

2.50

2.49

2.55

10.9

2.52

2.53

-500

HF

HF

HF

HF

HF

b.c.c, OJ + h.c.p.

Bl

Bl

Bl

Bl

1.2 Hex.

Tet. , a=12.1, c=3.7

Tet. , a=12.1, c=3.75

0.040 Tet. II, a=5.2, c=3.9

0.011 Perovskite, a=3.8

1.7

1.7

1.7

1.7

1.7

A15, a=5.1359

A15, a=5.134

A15, a=5.132

A15,. a=5.1302

A15, a=5.1315

A15, a=5.1334

A15, a=5.1345

A15, a=5.1354

A15, a=5.133

A15, a=5.134

A15, a=5.1345

A15, a=5.1547

A15, a=5.132

A15, a=5.133

477#

477

522

483

505^

483

517

505 v

505<7

500

472

500

500

5 38

544, 505,

525#, 5 31#

5 18 '7

529<7

505 V

503^

481

492

492

492

492

492

492

492

492

492

492

492

492

492

492
(VIII -19)

Material T

c

(°K) H (oersteds) T ** Crystal Structure co o n

J Ref.

Nb

3Pt0.10

Rh

0.90

Nb

3Pt0.30

Rh0.70

Nb

3Pt0.50

Rh

0.50

Nb

3Pt 0.70

Rh

0.30

Nb

3Pt

0.90

Rh

0.10

Nb

3Pt

0.95Rh0.05

Nb

3Pt0.98

Rh0.02

Nb Rh

Nb

3Rh

0.90

Ru0.10

Nb

3Rh

0.95Ru0.05

Nb

3Rh0.98

Ru

0.02

Nb_Sn

Nb^Sn (quenched)

Nb_Sn (sintered)

Nb0.5-0.83Sn0.5-0.17

(as cast)

Nb0.5-0.83Sn0.5-0.17

(annealed)

Nb3nTa„

Nb SnTa

Nb

2.5 SnTa

0.5 Sb2.759Bam

0.25

NbSnTaV

Nb

2SnTa

_ 5 V0. 5 NbSnV

Nb

2SnV

Nb

2 5 SnV

.5 Nb

Q ioTa

o 90 Nb

Q 5Ta

0.5 Nb

Q 025

T:L 0.975

Nb

Q 04Ti

96 Nb Ti

x y Ni

Np

2.8

5.1

6.25

7.4

7.9

8.9

9.6

2.64

2.44

2.42

2.42

18.0

4-16.7

17. 6M

17.95M

10.8

16.4

17.6

17.8

6.2

12.2

5.5

9.8

14.2

6.25

1.5

HF

HF

A15, a=5 1336

A15, a=5 1395

A15, a =5 1450

A15, a=5 1487

A15, a=5 1534

A15, a =5 160

A15, a=5 157

A15, a=5 1317

A15, a=5 1346

A15, a=5 135

A15, a=5 132

A15, a=5 289

A 15

A15, a=5.280

A15, a=5.289

A 15

A 15

A15, a=5.175

A 15

A15, a=5.115

A15, a=5.171

A 15

Hex.

0.35

0.41

°3Rb 0.27-0.29W 1.98 Hex. , a=7.4, c=7.

6

492

492

492

492

492

492

492

492

492

492

492

473

498

485

479

479

473

473

473

473

473

473

473

473

473

478

544

499

477 #

522

270

495

500
(VIII -20)

Material T

c (°K) H (oersteds) T ** Crystal Structure en o n

Ref

.

OTi

PPd

PPd

3.0-3.2

0.58

<0.35-0.7 DO

3.0

P

2Pd

P Pd (high temperature)

P Pd (low temperature)

P Pt

7 20 PRh„

PRu

PRu

2 Pa

Pb

PbRh„

PdS

Pd. _S (quenched)

Pd2.8

S

Pd.S

4 PdSb,

Pd0.63

Sb 0.37 ^uenched)

PdSc„

PdSe

Pd.Se

4 Pd

6 or 7 Se

Pd

17 Se

15 PdSn

Pd

2Sn

Pd

3Sn

2 PdTe

PdTe

1.02 PdTe

1.04 PdTe

PdTe

1.00

0.70

1.3

1.4

7.19

1.63

1.06

1.08

0.42

0.66

0.41

0.41

0.47-0.64

3.85

2.56

2.11

2.11

1.88

11 DO a=5.18, b=6.00,

c=7.46

Monoclinic, a=6.20, b=5.857 ! c=5.874,/=111.80°

481

491

491

491

Rhombohedral, a=7.28,

=f=110.12°

491

Complex 491

0. 35 491

CI, a=5.516 491

0, 35 491

0. 35 491

Tet. , a=3.925, c=3.238 504

47 6#

0. 32 489

0. 35 491

Cubic, a=8.93 491

0. 35 491

0. 32 Tet. , a=5.1147, c=5.5903 552

0. 35 491

0. 35 491

0. 32 E9 , a=12.442 469

0. 32 B34, a=6.727, c=6.912 552

Tet. , a=5.2324, c=5.6470 552

Similar to Pd.Te compound 552

0. 32 Cubic, a=10.606 552

B31, a=3.87, b=6.13, c=6.32 491

C37, a=8.12, b=5.65, c=4.31 491

B8

2

, a=4.399, c=5.666 491

B8

L

, a=4.152, c=5.670 552#

B8 , a=4.144, c=5.661 552

B8 a=4.143, c=5.659 552#

B8 a=4.138, c=5.652 552

B8 n) a=4.135, c=5.647 552
(VIII -21)

Material T ( K) H (oersteds) T ** Crystal Structure x> c ' o

v n Ref

.

PdTe„

PdTe2.1 PdTe2.3

pd l.lTe

Pd0.71

Te

0.,29

Pd Te

Pd

4Te

PdTh

2 Pd

5Th

Pd

3Y

p t V

Pt 0.87

S 0.13

PtSc

PtSc

4 Pt

3Sc

Pt- Sp 0.87 0.13

PtSn

PtSn

2 PtTe

PtTh

Pt

3Thy Pt

2Th

Pt.Th

Pt.Th

4 Pt

5Th

PtV

2.5 PtV.

PtV

1.69

1.89

1.85

4.07

0.40

0.76

0.85

0.37

0.59

0.44

0.98

3.5 Pt Y 0.42 0.58

3. 13

1. 36

2. 83

1. 26

0, 76*, 0. 33

C6, a=4.036, c=5.132

C6, a=4.037, c=5.128

C6, a=4.037, c=5.127

B8 a=4.152, c=5.671

X-ray evidence of Pd Te, Pd Te and Pd Te 3

X-ray evidence of Pd_Te,

Pd2 _ 5Te and Pd2Te J 0.32 Cubic,' a=12.674

0.32

0.32

0.3

C16, a=7.33, c=5.93

LI , a=4.076

B17-type + Pt

0.32 B2, a=3.268

0.32

0.32 LI a=3.958

Monoclinic PtSe^ on + Pt

B8-, a=4.11, c=5.44

0.34 CI, a=6.42

Ortho -rhombic, a=6.6144,

b=5.6360, c=11.865

B

f

, a=3.900, b=11.09,

c=4.454

D10 a=10.126, c=6.346

0.32

0.32

0.32

A 15

A 15

A 15

552

552

552

552

552

552

552

469

469

469

503*7

552

469

469

469

552

486

486

552

469

469

469

469

469

469

498

498

498

469

* Probably associated with Y.pto +++ Beginning of transition
(VIII -22)

Material T ( IO H (oersteds) T ** Crystal Structure X> c

' o n

Ref.

Pt Y

0.77 0.23

Pt Y 0.80 0.20

Pt

0. 77-0. 80Y

0. 23-0. 20

PtY

Pt Y

2 3 Pt Y

2.2 Pt

3Y

Pt Y

3 7 Pt Y

Pu

Rb

Re

Re Ti

x y Rh^

RhSc,

Rh0.24

Sc

0. 76

Rh0.25

Sc

0.,75 Rh

0.32

Sc

0. 63 Rh Sc

Rh

0.67

Te

0. 33 RhTh

Rh

2Th

Rh Th

Rh Th

Rh Ti

x y RhY

RhY„

RhY.

Rh

2Y

Rh

2Y

3 Rh

3Y

Rh

3Y

?

1.80

(portion only)

1.96

(portion only)

1.6-2.C

(portion

1 only)

0,.90

1.,70

0.82

1.9—7

0.92

(portion only)

0.88

(portion only)

0.49

0.36

1.07

0.65

1.48

1.07

0.32

C15, a=7.576

0.32 LI a=4.075

0.32

0.50

0.011

0.3

0.32

0.32

D10

2

, a=9.864, c=6.299

0.32

0.32 Ll

2

, a=3.898

B a=3.866, b=11.24,

c=4.22

0.32 LI,

0.32 B2, a=3.410

0.32

0.32 C15, a=7.489

C15, a=7.424

0.32 D10

2

, a=9.793, c=6.196

469

469

469

469

469

469

469

469

469

495

494

503^

522 503^

469

469

469

469

469

552

469

469

469

469

522

469

469

469

469

469

469

469
(VIII -2 3)

Material T (°K) H (oersteds) T ** Crystal Structure v Ref.

Rh

5Y 0.56 469

ruS 0.32 C2, a=5.609 552

RuSb 0.35 491

Ru

2Sb 0.35 491

RuSe„ 0.32 C2, a=5.934 552

RuTe„ 0.32 C2, a=6.391 552

Ru Ti 522

x y

Sb * 2.6-2.7 HF 520

SbSn 1.30-1.42, Bl or distorted Bl 470

1.42-2.37

Sb 0.01

V

0.99

3 ' 76 514#

Sb 0.02V

0.98

2.6-2.7

1. 30-•1.42,

1. 42-2.37

3..76

3. 29

2. 63

6.,75 + 6.95

7,,1

3,.2

2,.4

Sb 0.03

V0.97

2 " 53

Se (-130 kbar) « 6.75 + 6.95 Se II (unknown) 547

Si (-120-130 kbar) 7.1 540

O.Si Th 3.2 474

/^Si

2Th 2.4 474

C54, a=8.252, b=4.783, 522 c= 8.540

D8

a

, a=7.475, c=5.162 522

474

479

479

474

Tet., a=5.819, c=3.175 539

516v , 5 32^

A15, a=5.278 473

A15, a=5.041 473

A15, a=5.174 473

Bl 482

A

2

514#

A2 514#

A

2

514#

Si

2Ti

Si

3Ti5 SiV

3 17.1

Si0.1-0.38V

0.99-0.62

16. 7M

(as cast)

Sl0.1-0.38V0.99-0.62 16.95M

(annealed)

si

2w

3 2.8

p -Sn (quenched) 3.7 Sn?

SnTa„ 6.4

SnTaV

2 2.8

SnTa

2V 3.7

Sn Te (n=10.5-20xl02

°) x y ' .07-0.22

Sn0.02V

0.98

2.87

Sn0.04V0.96

1.86

Sn0.057

V0.943

-1.6

* Formed at 120 kbar, pre ssure removed at 77 K
(VIII -24)

Material

SnV

3 Ta

Ta

TaTa? (1100-<500o£)

Ta*7

1 0.025 0.975

Ta 0.05Ti

0.95

T

c (°K) H (oersteds) T ** Crystal Structure x> o n

Ref.

3.8

4.48

3.25-4.30

^bulk

1.3

2.9

Ta Ti

x y Tc0.05W

0.95

Tc W

0.10 0.90

1.25

Tc1 W

0.20 0.80

3.85

Tc W

0.30 0.70

5.75

Tc W

0.40 0.60

7.18

Tc W

0.50 0.50

7.52

Tc W

0.60 0.40

7.88

Te (-56,000 atm.) -3.3

Th 1.4 Ti 0.14

Ti 0.42

Ti

TiU

2 Ti V

0.70 0.30 6.14

Ti V

0.96 0.04 2.7

Ti V

0.975 0.025 1.4 TiV

Ti-Q 5Zr

5 (anneali=d) 1.23

Ti

0.5 Zr

0.5 ^uench(*-d) 2.0 TI 2.38

U

1.8 V 5.31*

A15, a=4.96

HF

HF

HF

HF

HF

56

176.5

HF

-0.8

Hex.

Hex.

Cubic, a=3.1617

Cubic, a=3.155 3

Cubic, a=3.147

Cubic, a=3.134

Cubic, a=3.126

<* + tracer", a=3.117

trace 3 +o~ , (cU-a=3.117,

(?j--a=9.520, c=5.003

C32, a=4.82, c=2.84

Cubic

Hex.

Cubic

473

505

519

525

505 7 ,529 7

503 v

499

499

522

524

524

524

524

524

524

524

510

504

523

490#

477 #

522

514#

477#

499

522

477

477

527 #

504

548

525

* Residual Resistivity Ratio = 27
(VIII -25)

Material T ( K) H (oersteds) T ** Crystal Structure & Ref.

c

' o

x nJ

w 0.012 1.070

w 0.005-0.011 ~1

WP" (various fi.1ms) 0.4-3.35

W<7 (-20-310$) 4.1M

Zr 0.65

Zr (annealed) 0.6

Zr 0.70 + 0.73

Zr (annealed) -0.46

493

526

0.012 A15 (when superconductive) 503 ^

541 7

Hex.,&;-Zr, a=5.03, c=3.12 549 W-Zr converted to*-Zr 549

=1 -Zr 549

551
(IX-1)

Table 3. High Magnetic Field Superconductive Materials and Some of Their Properties

(NOTE: All fields are quoted in kilo-oersteds. T , indicates temperature of measurement

degrees Kelvin. See text for discussion of field nomenclature.)

Material T

c cl Hc2 H

c3 obs

Ref.

Be^ -6.5 »11 550^

Bi II, Bi III (High fi eld data given) 437

C QK (Excess K)

o 0.55 0.160 (H1C) 0.32 494

0.55 0.730 (Hl/C) 0.32 494

C„K (Stoichiometric) 0.39 0.025 (H1C) 0.32 494

0.39 0.250 (HMC) 0.32 494

Inl-0.90

Pb

O-0.1

0.7-1.1 (Hc2,3

measured but quoted in ratio form) 480

In1.000Te

1.002

11 3.5-3.7 1.2 0. (extrapolated)

507 UA 6.5 0.15 ?25 1.3 534

La

3Se

4 8.6 0.2 >25 1.25 534

NNb

x y 13.5-17.0 <Hc2" some samples <38 kga uss) 483

N Nb Zr

x y z >130 4.2 517

Nb 9.15

9.15

1.710

2.020

4.2

1.4

531

531

Nb (unstrained) 1.1-1.8 3.40 6 .0-9 .1 4.2 538 Nb (strained) 1.25-1.92 3.44 6 .0-8 .7 4.2 538 Nb (cold drawn wire) 2.48 4.10 «10 4.2 538 NbV > 25 4.2 518

V

Nb-Sn (sintered) (Critical current density fields quoted) 485

^0.10^0.90 0.084 0.154 4.195 478

Sb* 2.6-2.7 4.4 1.55 520 Ta (99.95%) 0.090

0.275

0.325

0.425

0.375

1.175

1.425

1.850

3.72 2.66 2.27

1.30

519

519

519

519 TC0.30 W

0.70 5.75 7.5 4.2 524 Tc W

0.40 0.60 7.18 19.0 4.2 524 Tci W

0.50 0.50 7.52 29.0 4.2 524

Tc1 W

0.60 0.40 7.88 43.5 4.2 524

V 5.31 -0.80 -3.40 1.79 548 5.31 -0.75 -3.15 2. 548 5.31 -0.45 -2.20 3. 548 5.31 -0.30 -1.20 4. 548

* Formed at 120 kbar, pressure removed at 77°K.
(x-i)

BIBLIOGRAPHY

467. Lange, F. K. , J. Exp. Theor. Phys. 42, 42 (1962); Soviet Phys.

JETP 15, 29 (1962)

.

468. Taylor, A., Kagle, B. J., and Doyle, N. J., J. Less Common

Metals 5, 26 (1963).

469. Geballe, T. H. , Matthias, B. T. , Compton, V. B. , Corenzwit,

E. , Hull, G. W. Jr., and Longinotti, L. D. , Phys. Rev. 137 , A119-27 (1965).

470. Geller, S., and Hull, G. W. Jr., Phys. Rev. Letters 13,

127-9 (1964).

471. Geller, S., McWhan, D. B. , and Hull, G. W. Jr., Science 140 , 62-3 (1963).

472. Raub, C. J., Sweedler, A. R. , Jensen, M. A., Broadston, S.

,

and Matthias, B. T. , Phys. Rev. Letters 13, 746-7 (1964).

473. Cody, G. D. , Hanak, J. J., McConville, G. T. , and Rosi, F. D.

,

RCA Rev. 25, 338-41 (1964).

474. Hulm, J. K. , and Hardy, G., Third Internat. Conf. on Low Temp.

Phys. and Chem. , Houston, Texas, Dec. 1953 (MIT Library).

475. Caswell, H. L. , Solid State Comm. 2, 323-4 (1964).

476. Neighbor, J. E. , Cochran, J. F. , and Shiffman, C. A.,

Proc. 9th Int. Conf. on Low Temp. Physics, 479-81 (1965)

(ed. J. G. Daunt, D. 0. Edwards, F. J. Milford, M. Yaqub)

.

477. Bucher, E. , Heininger, F. , and Mu Her, J., See Ref. 476, p. 482-6

478. French, R. A., Lowell, J., and Mendelssohn, K. , See Ref. 476,

p. 540-3.
(X-2)

479. Kunz, W. , and Saur, E. , See Ref. 476, p. 581-3.

480. Gygax, S. , Olsen, J. L. , and Kropschot, R. H. , See Ref. 476,

p. 587-90.

481. Hulm, J. K. , Jones, C. K. , Mazelsky, R. , Miller, R. C.

,

Hein, R. A., and Gibson, J. W. , See Ref. 476, p. 600-3.

482. Hein, R. A., Gibson, J. W. , Allgaier, R. S., Houston, B. B. Jr.,

Mazelsky, R. , and Miller, R. C. , See Ref. 476, 604-6.

483. Gaule, G. K. , Breslin, J. T. , Ross, R. L. , Pastore, J. R.

,

and Shappirio, J. R. , See Ref. 476, p. 612-5.

484.V Adler, J. G. , and Ng, S. C, Canad. J. Phys. 43, 594-604 (1965).

485. Coles, G. W. , Corsan, J. M. , Buxton, A., and Lewis, B.

,

J. Less Common Metals 8, 402 (1965).

486. Hamilton, D. C. , Raub, C. J., Matthias, B. T. , Corenzwit, E.

,

and Hull, G. W. Jr., J. Phys. Chem. Solids (GB) 2_6, 665-7

(1965)

.

487. Luo, H. L. , Merriam, M. F. , and Hamilton, D. C, Science 145 , 581-3 (1964).

488. Merriam, M. F. , and Schreiber, D. S. , J. Phys. Chem. Solids

24, 1375-7 (1963).

489. Merriam, M. F. , Sweedler, A. R. , and Hamilton, D. C, Bull.

APS 9, 268 (1964).

490. Falge, R. L. Jr., Phys. Rev. Letters 11, 248-50 (1963).

491. Raub, C. J., Zachariasen, W. H. , Geballe, T. H. , and Matthias,

B. T. , J. Phys. Chem. Solids 24, 1093-1100 (1963).
(X-3)

492. Zegler, S. T. , Phys. Rev. 137, A1438-40 (1965).

493. Johnson, R. T. , Vilches, 0. E. , Wheatley, J. C. , and

Gygax, S., Phys. Rev. Letters 16, 101-4 (1966).

494. Hannay, N. B., Geballe, T. H. , Matthias, B. T. , Andres, K.

,

Schmidt, P., and Macnair, D. , Phys. Rev. Letters 14, 225-6

(1965).

495. Meaden, G. T. , and Shigi, T. , Cryogenics 4, 90-2 (1964);

also Meaden, G. T. , Cryogenics 4, 105-7 (1964).

496. Johnston, J. , Toth, L. , Kennedy, K. , and Parker, E. R.

,

Solid State Comm. 2_, 123 (1964).

497. Johnston, J. , U. of Cal. Berkeley, Lawrence Rad. Lab.

UCRL-11390 (1964).

498. Matthias, B. T. , Geballe, T. H. , Willens, R. H. , Corenzwit,

E., and Hull, G. W. Jr., Phys. Rev. 139, A1501 (1965).

499. Raub, C. J., and Zwicker, U. , Phys. Rev. 137, A142-3 (1965).

500. Sweedler, A. R. , Raub, C. J., and Matthias, B. T. , Phys.

Letters 15, 108-9 (1965).

501. Hein, R. A., Gibson, J. W. , Mazelsky, R. , Miller, R. C,

and Hulm, J. K. , Phys. Rev. Letters 12, 320-2 (1964).

502. Bommel, H. E. , Darnell, A. J., Libby, W. F. , and Tittman,

B. R. , Science 139, 1301-2 (1963).

503. V Bond, W. L. , Cooper, A. S., Andres, K. , Hull, G. W. , Geballe,

T. H., and Matthias, B. T. , Phys. Rev. Letters 15, 260-1 (1965)

504. Fowler, R. D. , Matthias, B. T. , Asprey, L. B. , Hill, H. H.

,

Lindsay, J. D. G. , Olsen, C. E. , and White, R. W. , Phys.

Rev. Letters 15, 860-2 (1965).
(X-4)

505.17 Gerstenberg, D. , and Hall, P. M. , J. Electrochem. Soc. Ill ,

936-42 (1964).

506. Geller, S., Jayaraman, A., and Hull, G. W. Jr., Appl. Phys.

Letters 4, 35-7 (1964).

507. Banus, M. D. , Hanneman, R. E. , Strongin, M. , and Gooen, K.

,

Science 142, 662-3 (1963).

508. Killpatrick, D. H. , J. Phys. Chem. Solids 25, 1213-6 (1964).

509. Killpatrick, D. H. , J. Phys. Chem. Solids 25, 1499-500 (1964).

510. Matthias, B. T. , and Olsen, J. L. , Phys. Letters 13, 201-2

(1964).

511. Merriam, M. F., Phys. Letters 9> 100-1 (1964).

512. Hauser, J. J., and Theuerer, H. C., Phys. Letters 14, 270-1

(1965)

.

513. Johnston, J., Toth, L. , and Parker, E. R. , UCRL-11317, p. 133-7

514. Pessall, N. , Gupta, K. P., Cheng, C. H. , and Beck, P. A.,

J. Phys. Chem. Solids 25, 993-1003 (1964).

515. Geller, S., Jayaraman, A., and Hull, G. W. Jr., J. Phys.

Chem. Solids 2_6, 35 3-61 (1965).

516.^ Alekseevskii, N. E., and Mikheeva , M. N. , Z. Eksper. i.

Teoret. Fiz. 38, 292-3 (1960).

517. Anderson, D. E. , Toth, L. E. , Rosner, L. G. , and Yen, C. M.

,

Appl. Phys. Letters 1_, 90-2 (1965).

518. D'Yakov, I. G. , Lazarev, B. G. , Matsakova, A. A., and

Ovcharenko, G. N. , Z. Eksper. i. Teoret. Fiz. 46, 831-2

(1964); Soviet Phys. JETP 19, 568-9 (1964).
(X-5)

519. Bots, G. J. C, Pals, J. A., Blaisse, B. S., DaJong, L. N. J.,

and Van-Engelen, P. P. J. , Physica 31, 1113-23 (1965).

520. McDonald, T. R. R. , Gregory, E. , Barberich., G. S. , McWhan,

D. B., Geballe, T. H. , and Hull, G. W. Jr., Phys. Letters

14, 16-7 (1965).

521. Caswell, H. L. , Phys. Letters 10, 44-5 (1964).

522. Zwicker, U. , Z. Metallkde, Dtsch. 54, 477 (1963).

523. Cape, J. A., Phys. Rev. 132, A1486-92 (1963).

524. Autler, S. H. , Hulm, J. K. , and Kemper, R. S., Phys. Rev.

140 , A1177-80 (1965).

525. Yun Lung Shen, L. , Senozan, N. M. , and Phillips, N. E.

,

Phys. Rev. Letters 14, 1025-7 (1965).

526. Gibson, J. W. , and Hein, R. A., Phys. Rev. Letters 12, 688

(1964)

.

527. van der Hoeven, B. J. C. Jr., and Keesom, P. H. , Phys. Rev.

135 , A631-7 (1964).

528. Rabenau, A., and Berben, T. J., Phys. Letters 12, 167 (1964).

529. Rairden, J. R. , and Neugebauer, C. A., Proc. IEEE 52, 1234-7

(1964)

.

530. Raub, C. J., and Webb, G. W. , J. Less Common Metals 5, 271-7

(1963).

531. Weber, R. , Phys. Rev. 133, A1487-92 (1964).

532.^ Artemenko, I. A., and Mikhailov, G. 0., Ukr. Fiz. Zh. £,

1369-71 (1964).
(X-6)

533. Alekseevskii, N. E. , Z. Eksper. i. Teoret. Fiz. 49, 159-62

(1965); Soviet Phys. JETP 22, 114-6 (1966).

534. Bozorth, R. M. , Holtzberg, F. , and Methfessel, S., Phys.

Rev. Letters 14, 952-3 (1965).

535. Raub, C. J., and Hamilton, D. C, J. Less Common Metals 6,

486-8 (1964).

536. Leslie, J. D. , Cappelletti, R. L. , and Ginsberg, D. M.

,

Phys. Rev. 134 , A309 (1964).

537. Phillips, N. E. , Phys. Rev. 134, A385 (1964).

538. Catterall, J. A., Williams, I., and Duke, J. F. , Brit. J.

Appl. Phys. 15, 1369-75 (1964).

539. Banus, M. D. , Vernon, S. N. , and Gatos, H. C. , J. Appl.

Phys. 36, 864 (1965).

540. Buckel, W. , and Wittig, J., Phys. Letters 17_, 187-8 (1965).

541.v Strongin, M. , Phys. Letters 17, 224-5 (1965).

542. Smith, T. F. , Phys. Rev. 137, A1435-7 (1965).

543. Rorer, D. C. , Onn, D. G. , and Meyer, H. , Phys. Rev. 138 , A1661 (1965).

544. McConville, T. , and Serin, B., Phys. Rev. Letters 13, 365-7 (1964)

545. Batterman, B. W. , and Barrett, C. S., Phys. Rev. Letters L3,

390-2 (1964).

546. Olsen, J. L. , Cryogenics 2, 356-8 (1962).

547. Wittig, J., Phys. Rev. Letters 15, 159 (1965).

548. Martin, R. B. , and Rose-Innes, A. C. , Phys. Letters 19,

467-9 (1965).
(X-7)

549. Tittman, B. , Hamilton, D. , and Jayaraman, A., J. Appl.

Phys. 35, 732-3 (1964).

550.^ Lazarev, B. G. , Semenenko, E. E. , and Sudovtsov, A. I.,

Z. Eksper. i. Teoret. Fiz. 45, 391-2 (1963); Soviet Phys.

JETP 18, 270-1 (1964).

551. Brandt, N. B. , and Ginzberg, N. I., Z. Eksper. i. Teoret.

Fiz. 46, 1216-9 (1964); Soviet Phys. JETP 19, 823-5 (1964).

552. Raub, C. J., Compton, V. B. , Geballe, T. H. , Matthias, B. T.

,

Maita, J. P., and Hull, G. W. Jr., J. Phys. Chem. Solids :26,

2051-7 (1965).
(XI -1)

REVIEW ARTICLES AND BOOKS ON SUPERCONDUCTIVITY

Onnes, H. Kamerlingh, Coramun. Kamerlingh Onnes Lab. 1_3, Supplement

34b (1913-14).

Crommelin, C. A., Physik. Zeitschr. 21, 274, 300, 331 (1920).

Meissner, W. , Metallwirtschaft 15, 289 (1930).

Schulze, A., Z. Ver. deut. Ing. 74, 149-52 (1930).

Bates, L. F., Science Progress 24, 565-72 (1930).

Meissner, W. , Metallwirtschaft 10, 289, 310 (1931).

DeHaas, W. J., and Voogd, J., Commun. Kamerlingh Onnes Lab. 20 , Supplement 73a (1932).

Clusius, K. , Zeits. Elektrochem. 38, 312-26 (1932).

Meissner, W. , Erg. Der Exakt. Naturw. 11, 219 (1932).

McLennan, J. C. , Nature 130, 879 (1932).

McLennan, J. C.., Pharm. J. 128, 470 (1932).

Kikoin, I., and Lazarev, B. , J. Tech. Phys. (USSR) 3, 237-54 (1933).

Meissner, W. , Physik. Zeitschr. 35, 931 (1934).

Tammann, G. , Z. Metallkunde 26, 61 (1934).

Burton, E. F. (Ed.), "The Phenomenon of Superconductivity," Univ.

of Toronto Press, Toronto (1934).

McLennan, J. C. , Reports on Prog, in Physics 1, 206 (1934).

McLennan, J. C, Roy. Soc. Proc. 15 2A , 1-46 (1935).

Meissner, W. , "Handbuch der Experimental Physik XI", Part 2, 204-262

(1935).

Smith, H. G., and Wilhelm, J. 0., Rev. Mod. Phys. 7, 237 (1935).

Darrow, K. K. , Rev. Sci. Instr. 7, 124 (1936).
(XI -2)

Ruhemann, M. , and Ruhemann, B. , "Low Temperature Physics," Cambridge

Univ. Press (1937).

Steiner, K. , and Grassmann, P., "Supra leitung," Vieweg und Sohn,

Brunswick (1937).

Silsbee, F. B. , J. Wash. Acad. Sci. 27, 225-44 (1937).

Shoenberg, D. , "Superconductivity," Cambridge Univ. Press (1938).

Shoenberg, D. , Uspekhi Fiz. Nauk. 19, 448-91; 20, 1-28 (1938).

Jackson, L. C. , Reports on Prog, in Physics 5, 335-44 (1939).

Burton, E. F. , Grayson Smith, H. , and Wilhelm, J. 0., "Phenomena

at the Temperature of Liquid Helium," Reinhold Publishing Corp.,

New York, pp. 87-123 (1940).

Casimir, H. B. G., Nederland. Tijdschr. Natuurkunde 8, 113-23 (1941).

Laue, M. Von, Ber. 75B, 1427-32 (1942).

Laue, M. Von, Physik. Z. 43, 274-84 (1942).

Mendelssohn, K. , Reports on Prog, in Physics IX), 358-77 (1944-45)

.

Itterbeek, A. van, Soc. Roy. beige ing. ind. , Mem. Ser B jL, 47-51

(1945)

.

Justi, E., Naturwiss. 33, 292-7, 329-33 (1946).

Ginsburg, V. L. , "Superconductivity," Academy of Science USSR,

Moscow, Leningrad (1946)

.

Hewlett, C. W. , G.E. Rev. 49, 19-25 (1946).

Andronikashvili, E. L. , and Tumanov, K. A., Uspekhi Fiz. Nauk. _33,

469-532 (1947).

Justi, E., "Leitfahigkeit und Leitungsmechanismus fester Stoffe,"

Gottingen, Vandenhoeck and Ruprecht, pp. 187-270 (1948).
(XI -3)

Laue, M. Von, Ann. Physik. 3, 40-2 (1948).

Meissner, W. , and Schubert, G. V., Fiat Rev. German Science (1939-46);

Physics of Solids Pt. II, 143-62 (1948).

Gorter, C. J., Physica 15, 55-64 (1949).

Mendelssohn, K. , Reports on Prog, in Physics 12, 270-290 (1948-49).

Vick, F. A., Science Progress 37, 268-74 (1949).

Wexler, A., Research, Lond. 3, 534 (1950).

Shoenberg, D. , Nuovo Cimento 10, Ser. IX, 459-89 (1953).

Unknown, Physica 19, 745-54 (1953).

Eisenstein, J., Rev. Mod. Phys. 26, 277 (1954).

Buckel, W. , Naturwiss. 42, 451 (1955).

Serin, B. , Handbuch Der Physik, Band XV, K^ltephysik II, SpringerVerlag, Berlin, pp. 210-73 (1956).

Zavaritskii, N. V., Priroda 45, 37-44 (1956).

Wexler, A., Metal. Progr. 69, 89 (1956).

Abrikosov, A. A., Vestnik Akademii Nauk SSSR #4, 30-36 (1958).

Boorse, H. A., Amer. Jour, of Physics 27, 47 (1959).

Buckel, W., Metall. 13, 814 (1959).

Cooper, L. N. , Amer. Jour, of Physics 28, 91 (1960).

Schoenberg, D. , "Superconductivity," (2nd Ed. , 1960 Printing)

,

Cambridge Univ. Press (1960); (1st Ed., 1938; 2nd Ed., 1952).

Bardeen, J., and Schrieffer, J. R. , Prog, in Low Temp. Phys. Vol. III.

Kropschot, R. H. , and Arp, V., Cryogenics 2_, 1 (1961).

Jones, W. H., Milford, F. J., and Fawcett, S. L. , J. of Metals 14,

836 (1962); Also Battelle Technical Review, (Sept. 1962).
(XI -4)

Lynton, E. A., "Superconductivity," Metheun and Co., London; John

Wiley & Sons, New York (1962). J *M

Tanenbaum, M. , and Wright, W. V. (Ed.), "Superconductors," John

Wiley & Sons, New York (1962).

Bardeen, J., Rev. Modern Phys. 34, 667 (1962).

Geballe, T. H. , and Matthias, B. T. , Ann. Rev. of Physical Chemistry,

Vol. 14 (1963).

Bowen, D. H. , "Effects of Pressure" in High Pressure Physics and

Chemistry Vol. I , R. S. Bradley (Ed.), Academic Press, London,

New York, pp. 355-73 (1963).

Bardeen, J. , "Superconductivity" in Advances in Materials Research

in the NATO Nations , MacMillan, New York, pp. 281-90 (1963).

Anderson, D. E. , "Superconductivity" in Magnetic Materials Digest

1964 , M. W. Lads, Philadelphia, pp. 196-217 (1964).

"Proc. Inter. Conf . on Science of Superconductivity, Hamilton, N.Y.

,

Aug. 1963," Rev. Mod. Phys. 36 (1964).

Geballe, T. H. , and Matthias, B. T. , "Superconductivity" in Annual

Review of Physical Chemistry Vol. 14 , pp. 141-160 (1964).

Lynton, E. A., "Superconductivity," Metheun & Co., London; John

Wiley & Sons, New York (1964).
(XII -1)

AUTHOR INDEX BY REFERENCE NUMBER

Adler, J. G. , 484

Adlhart, 0., 444

Alekseevskii, N. E. , 2-8, 56, 59, 60, 103, 153, 154, 158, 197,

269, 323, 326, 394, 427, 433, 516, 533

Allen, J. F., 86, 88, 99, 109, 111, 112

Allgaier, R. S. , 482

Anderson, D. E. , 517

Anderson, G. S. , 22, 227

Andres, K. , 494, 503

Andrews, D. H. , 49, 243

Androes, G. M. , 205

Andronikashvili, E. L. , 105

Aron, P. R., 321, 368

Arp, V. D., 189

Arrhenius, G. 0. S., 255, 449

Artemenko, I. A., 532

Aschermann, G. , 161, 306

Asprey, L. B. , 504

Atoji, M. , 100

Autler, S. H. , 334, 524

Bala, V. B. , 128

Banus, M. D. , 277, 507, 539

Barberich, G. S. , 520

Baron, V. V. , 323

Barrett, C. S. , 545
(XII -2)

Barth, N. , 78, 354

Batterman, B. W. , 545

Bayles, B. , 419

Bean, C. P., 331

Beck, P. A., 195, 330, 514

Beenakker, J. J. M. , 297

Bender, D. , 417

Benesovsky, F. , 447

Berben, T. J., 528

Bergeron, C. J. , 429

Berghout, C. W. , 358

Berlincourt, T. G. , 126, 157, 194, 218, 252, 268, 290, 349, 399, 466

Berman, A. , 92

Betz, C. , 288

Binkert, T. , 415

Blaisse, B. S. , 519

Blanpain, R. , 162

Blaugher, R. D. , 181, 182, 207, 216, 217, 253, 266, 275, 300, 327,

369, 432, 452, 453, 464

Blumberg, R. H. , 332, 367

Boato, G., 436

Bohm, H. V., 250

Boiler, H. , 370

Bommel, H..E., 424, 442, 502

Bond, W. L. , 503
(XII -3)

Bondar, V. V., 197, 394

Bon Mardiem, G. , 356

Boom, R. W. , 429

Boorse, H. A., 92, 231, 343, 344

Bots, G. J. C. , 519

Bowman, A. L. , 271, 397

Bozorth, R. M. , 174, 186, 187, 247, 534

Brandt, N. B. , 8, 203, 437, 551

Breslin, J. T. , 483

Broadston, S., 472

Brucksch, W. F. Jr., 49

Bryant, C. A. , 206, 389

Bucher, E. , 130, 274, 275, 293, 295, 415, 417, 418, 448, 477

Buckel, W., 77, 95, 152, 183, 213, 214, 353, 438, 459, 540

Budnick, J. I., 188, 209, 375

Buehler, E. , 365, 384

BUlow, H. , 213

Bundy, F. P. , 304

Bums, M. J. , 450

Busch, G., 121, 130, 366

Buxton, A. , 485

Callen, E. , 338

Calverley, A., 170, 244

Cape, J. A. , 523

Cappelletti, R. L. , 536
(XII -4)

Carpenter, J. H. , 312

Carruthers, J. A., 132

Casimir-Jonker, J. M. , 74

Caswell, H. L. , 378, 379, 475, 521

Catterall, J. A. , 538

Chandra sekhar, B. S., 21, 134, 275, 455

Chanin, G. , 319

Cheng, C. H. , 195, 330, 514

Chester, P. F. , 199

Chiou, C. , 320

Chotkevich, I. D. , 106

Chotkewitsch, W. I., 80

Chou, C, 323, 233

Clogston, A.M., 364

Clusius, K. , 85

Cobble, J. W., 163

Cochran, J. F., 148, 193, 371, 476

Cody, G. D., 185, 298, 473

Coles, B. R. , 256, 257, 265, 456

Coles, G. W., 485

Compton, V. B. , 41, 93, 127, 142, 173, 202, 212, 224, 239, 270,

279, 454, 469, 552

Connel, R. A. , 342

Connolly, A. , 132

Cook, D. B., 343, 344
(XII -5)

Cooper, A. S. , 503

Cooper, J. L. , 298

Corak, W. S. , 16

Corenzwit, E. , 25, 28, 32, 34, 35, 93, 115, 116, 125, 128, 142,

172, 173, 184, 196, 200, 201, 202, 211, 223, 224, 239, 247,

275, 283, 352, 364, 454, 469, 486, 498

Corsan, J. M. , 485

Croft, A. J., 374

Curry, M. A. , 339

Dabbs, J. W. I., 47

Darby, J. B. Jr., 64, 102, 408

Darnell, A. J., 424, 442, 502

Daunt, J. G., 45, 163, 166, 168

Davis, D. D., 174, 186, 187, 247

DeBoer, J., 73

Debruyn Ouboter, R. , 297

Decker, D. L. , 159

DeHaas, W. J., 15, 70, 71, 72, 73, 74, 87, 90, 281, 381, 402, 403

DeJong, L. N. J., 519

DeSorbo, W. , 190, 248, 441

Devlin, G. E. , 196

D'Heurle, F. M. , 430

Dickson, C. C. , 370

Dillinger, J. R. , 192
(XII -6)

Doidge, P. R., 309

Dorsi, D. , 310

Douglas, D. H. , 332

Doulat, J. , 382

Downey, J. W. , 102

Doyle, M. V., 331

Doyle, N. J. , 468

Druyvesteyn, W. F. , 357, 407

Duke, J. F. , 538

Dummer, G. , 438, 459

Dunaev, J. A. , 307

D'Yakov, I. G. , 518

Efimov, Yu. V., 323

Eisenstein, J. , 1

Fairbank, H. A. , 179

Falge, R. L. , 172, 363, 490

Finnemore, D. K. , 249

Fisk, Z., 256

Floyd, R. , 9

Fortmann, J. , 353

Fowler, R. D. , 504

Franck, J. P., 380

Franz, H. , 20, 69, 83, 84, 89, 123

French, R. A. , 478
(XII -7)

Friederich, E. , 306

Fukuroi, T. , 462

Gager, J. G. , 166

Gaidukov, Yu. P. , 60

Galasso, F. , 409, 419, 420

Gallinaro, G. , 436

Galkin, A. , 405

Gatos, H. C, 277, 311, 355, 539

Gaule, G. K., 444, 483

Gayley, R. I. Jr. , 341

Geballe, T. H. , 34, 184, 207, 211, 223, 224, 236, 239, 259, 270,

283, 292, 454, 469, 491, 494, 498, 503, 520, 552

Geiser, R. , 435

Geller, S., 34, 54, 58, 124, 140, 141, 238, 285, 470, 471, 506,

515

Gendron, M. F. , 229

Gerber, J. F. , 313

Gerstenberg, D. , 505

Gey, W., 440, 459

Gibson, J. W. , 223, 369, 431, 432, 446, 452, 464, 481, 482, 501,

526

Ginsberg, D. M. , 536

Ginzberg, N. I., 203, 392, 437, 551

Giorgi, A. L. , 271, 278, 284, 397
(XII -8)

Glagoleva, V. P., 55, 61, 62

Goldstein, R. , 124

Golik, V. R., .346

Gomes De Mesquita, A. H. , 461

Goodman, B. B. , 23, 29, 177, 356, 372, 382, 390, 435

Gooen, K. H. , 334, 507

Grassman, P. , 348

Gregory, E. , 520

Gschneider, K. A. Jr., 234

Guenault, A.M., 361

Guggenheim, J. , 301

Gupta, K. P. , 330, 514

Guttman, L. , 13, 44, 51, 92

Gygax, G. , 118

Gygax, S., 480, 493

Hagner, R. , 299, 315

Hake, R. R. , 126, 178, 194, 218, 252, 268, 289, 335, 399, 466

Haley, F. C, 243

Hall, P. M. , 505

Hamilton, D. C. , 449, 486, 487, 489, 535, 549

Hanak, J. J., 185, 298, 473

Hannay, N. B. , 494

Hanneman, R. E. , 507

Hardy, G. F. , 10, 42, 474
(XII -9)

Hart, H. R. Jr. , 303, 434

Hat ton, J. , 64, 65

Hauser, J. J., 317, 512

Heaton, J. W. , 428

Hein, R. A., 27, 30, 31, 135, 151, 167, 172, 223, 228, 300, 363,

369, 431, 432, 446, 452, 464, 481, 482, 501, 526

Heiniger, F. , 276, 295, 415, 448, 477

Heller, W. R. , 430

Hennig, G. , 46

Henry, W. E. , 27, 288

Herbstein, F. H. , 241

Hernandez, H. P. , 321

Hill, H. H., 504

Hillairet, J., 177

Hilsch, R. , 77, 183, 213, 215, 296

Hinrichs, C. H. , 324

Hirshfeld, A. T. , 231

Hitchcock, H. C. , 368

Holleck, H. , 447

Holtzberg, F. , 534

Hopkins, D. C, 180, 219

Horn, F. H. , 49, 97

Horwitz, N. H. , 250

Housto, B. B. Jr., 482

Howlett, L. E., 113
(XII -10)

Hsu, F. S. L. , 310, 365, 384

Hudson, R. P. , 423

Hull, G. W. Jr., 184, 211, 224, 239, 283, 454, 469, 470, 471, 486,

498, 503, 506, 515, 520, 552

Hulliger, F., 301, 413, 414

Hulm, J. K., 10, 11, 21, 29, 42, 43, 48, 134, 136, 182, 207, 216,

217, 221, 253, 266, 275, 300, 327, 431, 455, 474, 481, 501,

524

Ittner, W. B. Jr. , 122

Jacobs, I. S. , 434

Jansen, H. G. , 139, 242

Jayaraman, A., 506, 515, 549

Jennings, L. D. , 325

Jensen, M. A. , 257, 472

Johnson, R. T. , 493

Johnston, H. L. , 232, 233

Johnston, J., 496, 497, 513

Joiner, W. C. H. , 453

Jones, C. K. , 455, 481

Jones, G. 0. , 199

Jones, R. E. , 122, 229

Jurriaanse, T. , 281, 282

Justi, E., 66, 119, 161, 245, 306, 451

Kagle, B. J. , 468
(XII -11)

Kasper, J. S., 304, 305

Keesom, P. H. , 24, 206, 272, 389, 527

Kemper, R. S. , 524

Kennedy, K. , 496

Kertes, L. , 51

Khotkevich, V. I., 346, 401

Khukhareva, I. S. , 387

Killpatrick, D. H. , 508, 509

Knight, W. D. , 205

Koch, D. , 460

Kolbe, C. L., 434

Kostina, T. I., 8

Kramer, J. , 306

Kropschot, R. H. , 189, 480

Kunz, W. , 479

Kunzler, J. E. , 310, 365, 383, 384

Kurti, N. , 12

Kushmin, R. N. , 198

Kuz'min, R. N. , 155, 237, 286, 287

Lacaze, A. , 356

LaFleur, W. J., 311

Lam, D. J. , 102

Lane, C. T. , 14

Lange, F. , 147
(XII -12)

Langereis, C. , 461

Lautz, Von G. , 96, 263, 264

Lawrence, P. E. , 434

Lazarev, B. G. , 81, 101, 144, 346, 395, 405, 518, 550

LeBlanc, M. A. R. , 400

Leenhouts, J. I., 461

Legvold, S., 22, 227, 339

Leslie, D. H. , 126, 194, 268, 289, 399

Leslie, J. D. , 536

Leupold, H. A., 231

Lewis, B. , 485

Libby, W. F. , 424, 442, 502

Lifanov, L. I., 6, 56

Lindsay, J. D. G. , 504

Little, W. A. , 400

Livingston, J. D. , 322, 457, 458

Lock, J. M. , 235

Longinotti, L. D. , 469

Lounasmaa, 0. V., 291

Love, W. F., 36, 189, 338

Lowell, J., 478

Luo, H. L., 487

Lutes, 0. S. , 160

Lynton, E. A., 318, 319, 340, 341, 345
(XII -13)

Macnair, D. , 494

Malta, J. P., 202, 310, 465, 552

Mapother, D. E. , 148, 159, 180, 193, 219, 249, 267, 329, 336, 337

Marchand, J. F. , 393

Martienssen, W. , 215

Martin, D. L. , 380, 421

Martin, R. B. , 548

Matsakova, A. A., 518

Matthias, B. T. , 11, 19, 25, 28, 32, 33, 34, 35, 37, 38, 39, 43,

48, 54, 93, 94, 115, 116, 117, 124, 127, 128, 137, 138, 140

142, 146, 171, 172, 173, 184, 186, 200, 201, 202, 204, 207,

211, 212, 216, 223, 224, 234, 236, 239, 240, 246, 247, 270,

271, 275, 280, 283, 292, 352, 364, 422, 449, 454, 469, 472,

486, 491, 494, 498, 500, 503, 504, 510, 552

Maxwell, E. , 160

Mazelsky, R. , 481, 482, 501

McConville, G. T. , 185, 473, 544

McDonald, T. R. R. , 520

McLachlan, D. , 340

McLennan, J. C, 86, 99, 109, 111, 112, 113, 308

McWhan, D. B. , 471, 520

Meaden, G. T. , 226, 495

Meissner, H. , 26, 294

Meissner, W. , 20, 69, 75, 76, 83, 84, 89, 123, 273, 404
(XII -14)

Mendelssohn, K. , 98, 170, 360, 478

Mendoza, E. , 17, 390

Merriam, M. F., 255, 256, 257, 258, 260, 261, 445, 487, 488, 489,

511

Methfessel, S., 534

Meyer, H. , 543

Meyer, L. , 46

Michailov, N. N. , 326, 427

Migunov, L. , 103

Mikhailov, G. 0. , 532

Mikhailov, Yu. G. , 131

Mikheeva, M. N. , 516

Miller, C. E. , 35

Miller, R. C. , 431, 481, 482, 501

Milne, J. G. C, 175

Mingazin, T. A., 53

Minnigerode, G. Von, 183, 191, 296

Moore, J. R. , 98

Morin, F. J., 202, 310, 465

Mould, R. E., 337

Muheim, J., 293, 448

Muir, H., 288

Mliller, C. , 359

Muller, J., 121, 130, 274, 276, 293, 295, 301, 314, 328, 366,

412, 413, 414, 415, 416, 417, 418, 448, 477
(XII -15)

Nakhutin, I. E. , 81

Neighbor, J. E. , 476

Netzel, R. G. , 192

Neugebauer, C. A., 529

Ng, S. C, 484

Nichols, G. E., 190, 248

Nikulin, E. I., 131

Niven, C. D. , 308

Nix, F. C. , 338

Norman, M. , 135

Norton, L. J. , 102

Novick, D. T. , 375

Nowotny, H. , 447

Ohtsuka, Y. , 462

Olsen, C. E. , 504

Olsen, J. L. , 480, 510, 546

Onn, D. G. , 543

Onnes, K. , 91

Opitz, W. , 351

Otter, F. A. , 336

Otto, G. , 460

Ovcharenko, G. N. , 518

Pablo, M. R. , 464

Pals, J. A. , 519

Parker, E. R. , 496, 513
(XII -16)

Parthe, E., 370

Pastore, J. R. , 483

Pearson, W. B. , 108

Pessall, N. , 514

Peter, M. , 364

Phelan, R. , 189

Phillips, N. E., 156, 422, 525, 537

Pickles imer, M. L. , 230

Pincus, A. G. , 331

Polukarov, P. M. , 197, 394

Pyle, J., 409

Quinn, D. J., 209, 320

Rabenau, A., 528

Raetz, K., 254

Rairden, J. R. , 529

Raub, C. J., 259, 260, 262, 449, 472, 486, 491, 499, 500, 530, 535, 552

Rayl, M. , 298

Rayne, J. A., 300

Reeber, M. D. , 143

Reed, T. B. , 277, 311, 355

Reif, F. , 251

Reinmann, R. , 416

Reinov, H. M. , 131

Renard, M. , 362, 382
(XII -17)

Reynolds, J. M. , 14

Rhoderick, E. H. , 347

Rinderer, L. , 348

Risi, M. , 328

Rizzuto, C. , 436

Rjabinin, J. N. , 80, 82, 106, 401

Roberts, B. W. , 303

Roberts, L. D. , 47

Roddy, J. T., 311

Rogener, H. , 63

Rollin, B. V., 64, 65

Rorer, D. C. , 543

Rose, R. M. , 225

Rose-limes, A. C, 244, 410, 428, 548

Rosenblum, E. S. , 334

Rosi, F. D. , 185, 473

Rosier, U. , 222, 398

Rosner, L. G. , 517

Ross, R. L. , 444, 483

Rothwarf , F. , 370

Rowel 1, P.M., 170

Rlihl, W., 376

Samsonov, G. V., 333, 433

Saur, E. J., 139, 254, 299, 315, 359, 386, 460, 479
(XII-18)

Savitskii, E. M. , 323

Schepelev, J. D. , 80, 401

Schirber, J. E. , 100, 114, 176

Schmidt, P. , 494

Schneider, D. , 263, 264

Schreiber, D. S. , 488

Schroder, E. , 96, 110

Schubert, K. , 222, 398

Schubnikow, L. W. , 80, 82

Schulitsova, 0. I., 433

Schult, P., 386

Schwidtal, K. , 296, 377, 463

Scott, R. B. , 391

Seidel, G. , 24

Sekula, S. T. , 230, 429

Sellmaier, A. , 79

Semenenko, E. E., 144, 395, 550

Senozan, N. M. , 525

Seraphim, D. P., 169, 320, 342, 367, 375, 430

Serin, B., 318, 319, 341, 345, 544

Sevastyanov, B. K. , 373

Seymour, E. F. W. , 65

Shalnikov, A. I. , 392

Shappirio, J. R. , 483
(XII -19)

Sharvin, G. , 104

Shaw, R. W. , 159, 180

Sherwood, R. C. , 364

Shibuya, Y. , 462

Shiftman, C. A., 360, 476

Shigi, T., 495

Shiraashek, E., 385

Shoenberg, D. , 120, 164, 165

Shubnikov, L. V., 106, 401

Simon, F. , 12

Smirnov, A. P., 101, 131

Smirnova, E. M. , 396, 411

Smith, T. F., 542

Smith, T. S., 45, 166, 168

Snider, J. W. , 208

Soehle, S. , 419

Soklakov, A. I. , 155

Spedding, F. H. , 22, 227, 339

Spry, R. J. , 208

Steele, M. G. , 30, 167

Stepanova, A. A., 129

Storms, E. K. , 271, 397

Stout, J. W. , 13, 44

Strongin, M. , 179, 507, 541
(XII-20)

Sudovtsov, A. I., 101, 144, 395, 550

Suhl, H., 93, 115, 116, 200, 201, 247

Suits, J. C, 443

Swartz, P. S. , 316

Sweedler, A. R. , 472, 489, 500

Swenson, C. A., 100, 114, 176, 324, 325

Szklarz, E. G. , 271, 278, 284, 397

Taconis, K.' W. , 297

Taylor, A. , 266, 468

Templeton, I. M. , 150

Theuerer, H. C. , 512

Thomas, J. G. , 17

Thompson, C. T. , 313

Thomson, J. , 456

Tittman, B. R. , 424, 442, 502, 549

Toth, L. , 496, 513, 517

Toxen, A.M., 210, 450

VanAlphen, P. M. , 72

VanAubel, E., 15, 70, 71, 87, 381

VanBeelen, H. , 297

van der Hoeven, B. J. C. Jr., 527

Van-Engelen, P. P„ J., 519

VanOoijen, D. J., 357, 407

VanReuth, E. C, 330
(XII -21)

VanVucht, J. H. N. , 407

Veal, B. W. , 300

Venema, A. , 393

Vernon, S. N. , 539

Veyssie, J. J. , 177

Vieweg, G. , 66

Vilches, 0. E. , 493

Voigt, B. , 273

von Herzen, M. , 261

Voogd, J., 15, 70, 71, 87, 90, 381, 402, 403

Webb, G. W. , 530

Weber, R. , 531

Wei, C. T., 195

Weill, L., 177, 382

Wentorf , R. H. , 305

Wernick, J. H. , 204, 310, 365, 406

Westerhoff, H. , 20, 83, 84, 89

Wexler, A. , 16

Wheatley, J. C, 493

White, D., 232, 233

White, G. K., 133

White, P. R. , 384

White, R. W. , 504

Whitehead, C. S. , 350

Wiedemann, W. , 149
(XII -22)

Wiederhold, E. W. , 208

Wilhelm, J. 0., 86, 109, 111, 112, 113, 308

Willens, R. H. , 498

Williams, A. J., 174, 187

Williams, H. J., 364

Williams, I. , 538

Wilson, J. H., 189

Wittig, J., 540, 547

Wolcott, N. M. , 27, 135, 151, 302

Wolgast, R. C. , 321

Wood, E. A., 41, 128, 137, 142

Woods, S. B. , 133

Woolf, M. A. , 251

Wulff, J., 225

Yasukochi, K. , 426

Yen, C. M. , 517

Yencha, A. J. , 442

Young, R. A., 9, 18, 40, 67

Yun Lung Shen, L. , 525

Zachariasen, W. H. , 25, 146, 491

Zavaritskii, N. V., 220, 388

Zegler, S. T. , 408, 492

Zemansky, M. W. , 92, 343, 344

Zhdanov, G. S., 53, 55, 57, 59, 61, 62, 107, 145, 153, 155, 1|8,

198, 237, 286, 287, 396
(XII -2 3)

Zhuravlev, N. N. , 6, 50, 51, 52, 53, 57, 59, 107, 129, 145, 153, 155,

158, 198, 396, 411, 425

Ziegler, W. T. , 9, 18, 40, 49, 67, 68, 97

Zucker, M. , 318

Zwicker, U. , 499, 522

Zyvzin, N. I. , 129

U.S. GOVERNMENT PRINTING OFFICE: 1966 —251-020/31

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WASHINGTON, O.C. 20230

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