Abstract:
The present invention provides a method and system to simultaneously use the microwave and Zeeman end resonances associated with the same sublevel of maximum (or minimum) azimuthal quantum number m to lock both the atomic clock frequency and the magnetic field to definite values. This eliminates the concern about the field dependence of the end-resonance frequency. In an embodiment of the system of the present invention, alkali metal vapor is pumped with circularly-polarized D 1  laser light that is intensity-modulated at appropriate resonance frequencies, thereby providing coherent population trapping (CPT) resonances. In another embodiment, pumping with constant-intensity circularly-polarized D 1  laser light enhances magnetic resonances that are excited by alternating magnetic fields oscillating at appropriate resonance frequencies. In both embodiments, the resonances are greatly enhanced by concentrating most of the atoms in the initial state of the resonances, and by diminishing the spin-exchange broadening of the resonances. This leads to greater stability of optically pumped atomic clocks. This invention can also be used to operate an atomic magnetometer, where the feedback signal used to stabilize the magnetic field at the alkali-vapor cell can serve as a sensitive measure of the ambient magnetic field.

Description:
CROSS REFERENCE TO RELATED APPLICATION  
       [0001]    This application claims priority to U.S. Provisional Application No. 60/462,035, filed on Apr. 11, 2003, the disclosure of which is hereby incorporated by reference in its entirety. 
     
    
     
       BACKGROUND OF THE INVENTION  
         [0002]    1. Field of the Invention  
           [0003]    The present invention relates to the field of optically pumped atomic clocks or magnetometers, and more particularly to atomic clocks or magnetometers having simultaneous locking of field and frequency with end resonances.  
           [0004]    2. Description of the Related Art  
           [0005]    Conventional, gas-cell atomic clocks utilize optically pumped alkali-metal vapors. Atomic clocks are utilized in various systems which require extremely accurate frequency measurements. For example, atomic clocks are used in GPS (global positioning system) satellites and other navigation and positioning systems, as well as in cellular phone systems, scientific experiments and military applications.  
           [0006]    In one type of atomic clock, a cell containing an active medium, such as rubidium or cesium vapor, is irradiated with both optical and microwave power. The cell contains a few droplets of alkali metal and an inert buffer gas at a fraction of an atmosphere of pressure. Light from the optical source pumps the atoms of the alkali-metal vapor from a ground state to an optically excited state, from which the atoms fall back to the ground state, either by emission of fluorescent light or by quenching collisions with a buffer gas molecule like N 2 . The wavelength and polarization of the light are chosen to ensure that some ground state sublevels are selectively depopulated, and other sublevels are overpopulated compared to the normal, nearly uniform distribution of atoms between the sublevels. It is also possible to excite the same resonances by modulating the light at the Bohr frequency of the resonance, as first pointed out by Bell and Bloom, W. E. Bell and A. L. Bloom,  Phys. Rev.  107, 1559 (1957), hereby incorporated by reference into this application. The redistribution of atoms between the ground-state sublevels changes the transparency of the vapor so a different amount of light passes through the vapor to a photo detector that measures the transmission of the pumping beam, or to photo detectors that measure fluorescent light scattered out of the beam. If an oscillating magnetic field with a frequency equal to one of the Bohr frequencies of the atoms is applied to the vapor, the population imbalances between the ground-state sublevels are eliminated and the transparency of the vapor returns to its unpumped value. The changes in the transparency of the vapor are used to lock a clock or magnetometer to the Bohr frequencies of the alkali-metal atoms.  
           [0007]    The Bohr frequency of a gas cell atomic clock is the frequency v with which the electron spin S processes about the nuclear spin I for an alkali-metal atom in its ground state. The precession is caused by the magnetic hyperfine interaction. Approximate clock frequencies are v=6.835 GHz for  87 Rb and v=9.193 GHz for  133 CS. Conventionally, clocks have used the “0-0” resonance which is the transition between an upper energy level with azimuthal quantum number m=0 and total angular momentum quantum number f=I+½, and a lower energy level, also with azimuthal quantum number m=0 but with total angular momentum quantum number f=I−½.  
           [0008]    For atomic clocks, it is important to maintain the minimum uncertainty, δv, of the resonance frequency v. The frequency uncertainty is approximately given by the ratio of the resonance linewidth, Δv, to the signal-to-noise ratio, SNR, of the resonance line. That is, δv=Δv/SNR. Clearly, one would like to use resonances with the smallest possible linewidth, Δv, and the largest possible signal-to-noise ratio, SNR.  
           [0009]    For miniature atomic clocks it is necessary to increase the density of the alkali-metal vapor to compensate for the smaller physical path length through the vapor. The increased vapor density leads to more rapid collisions between alkali-metal atoms. These collisions are a potent source of resonance line broadening. While an alkali-metal atom can collide millions of times with a buffer-gas molecule, like nitrogen or argon, with no perturbation of the resonance, every collision between alkali-metal atoms interrupts the resonance and broadens the resonance linewidth. The broadening mechanism is “spin exchange,” the exchange of electron spins within a pair of alkali-metal atoms during a collision. The spin-exchange broadening puts fundamental limits on how small such clocks can be. Smaller clocks require larger vapor densities to ensure that the pumping light is absorbed in a shorter path length. The higher atomic density leads to larger spin-exchange broadening of the resonance lines, and makes the resonance lines less suitable for locking a clock frequency or a magnetometer frequency.  
           [0010]    U.S. Pat. No. 2,951,992 describes an atomic frequency standard having a pair of cells of alkali metal vapor in which a substantially homogenous static magnetic field permeates both cells and energy of a sum frequency of a frequency source and an interpolation generator is applied to one cell to excite hyperfine ground energy level transitions therein, and energy of a difference frequency of same frequency source and same interpolation generator is applied to the other of the cells to excite microwave hyperfine energy level transitions in the other cell.  
           [0011]    It is desirable to provide a method and system for using end resonances for providing simultaneous locking of field and frequency in the same cell in order to eliminate most of the sensitivity to field differences between the two cells, and to operate atomic clocks at much higher densities of alkali-metal atoms than conventional systems.  
         SUMMARY OF THE INVENTION  
         [0012]    Co-pending U.S. patent application Ser. No. 10/620,159, hereby incorporated by reference in its entirety into this application, relates to a method and system for using end resonances of highly spin-polarized alkali metal vapors for an atomic clock, magnetometer or other system. A left end resonance involves a transition from the quantum state of minimum spin angular momentum along the direction of the magnetic field. The traditional 0-0 resonance and the end resonances of  87 Rb vapor are shown in FIG. 1.  
           [0013]    A right end resonance involves a transition from the quantum state of maximum spin angular momentum along the direction of the magnetic field. For each quantum state of extreme spin there are two end resonances, a microwave resonance and a Zeeman resonance. For  87 Rb, the microwave end resonance occurs at a frequency of approximately 6.8 GHz and for  133 CS the microwave end resonance frequency is approximately 9.2 GHz. The Zeeman end resonance frequency is very nearly proportional to the magnetic field. For  87 Rb the Zeeman end resonance frequency is approximately 700 kHz/G, and for  133 CS the Zeeman end resonance frequency is approximately 350 kHz/G. It is desirable to use left and right microwave end resonances for an atomic clock. The fundamental problem is that the right end resonance requires the atoms to be in states with the maximum possible azimuthal quantum number m=I+½ and the left end resonance requires the atoms to be states with the minimum possible azimuthal quantum number m=−I−½. The present invention provides a method and apparatus for simultaneously exciting a microwave end transition and a Zeeman end transition with doubly-modulated laser light or with alternating magnetic fields, oscillating at the frequencies of both transitions, and setting the ratios between the obtained signal frequencies and the local oscillator frequency to preset integer values, thereby locking both the local-oscillator frequency and the total magnetic field at the alkali-vapor cell.  
           [0014]    The present invention provides a method and system to simultaneously use the microwave and Zeeman end resonances associated with the same sublevel of maximum (or minimum) azimuthal quantum number m to lock both the clock frequency and the total magnetic field to definite values. This eliminates the concern about the magnetic-field dependence of the end-resonance frequency. In one embodiment of the system of the present invention, alkali metal vapor is pumped with circularly polarized D 1  laser light that is intensity modulated at appropriate resonance frequencies, thereby providing coherent population trapping (CPT) resonances, that can be observed as an increase in the mean transmittance of the alkali-metal vapor. In a closely related embodiment, circularly polarized pumping light of fixed intensity is used to pump the atoms into the right (or left) end state, depending on the helicity of the light, and the resonances are excited by magnetic fields oscillating at the microwave and Zeeman end-resonance frequencies.  
           [0015]    The invention will be more fully described by reference to the following drawings. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0016]    [0016]FIG. 1 is a graph of  87 Rb ground-state energy levels and resonances.  
         [0017]    [0017]FIG. 2 is a schematic diagram of a system of operating an atomic clock in accordance with the teachings of the present invention.  
         [0018]    [0018]FIG. 3 is a flow diagram of a method of operating an atomic clock in accordance with the teachings of the present invention.  
         [0019]    [0019]FIG. 4 is a graph of qualitative time dependence of light intensity, simultaneously modulated at the resonance frequencies of the Zeeman and microwave end transitions.  
         [0020]    [0020]FIG. 5 is a plot of δB, uncertainty of the magnetic field, and δv q , uncertainty of the local oscillator frequency, for intersection of locking ridges for Zeeman and microwave resonances within an error parallelogram.  
         [0021]    [0021]FIG. 6 is s graph of trajectories in δB-δv q  plane for locking the field B and frequency v q  for: (a) ridge-climbing combinations; and (b) for simple modulation of B for locking to the Zeeman end resonance, and v q  for locking to the microwave end resonance.  
         [0022]    [0022]FIG. 7 is a flow diagram of a method for adjusting the local oscillator frequency and the magnetic field. 
     
    
     DETAILED DESCRIPTION  
       [0023]    Reference will now be made in greater detail to a preferred embodiment of the invention, an example of which is illustrated in the accompanying drawings. Wherever possible, the same reference numerals will be used throughout the drawings and the description to refer to the same or like parts.  
         [0024]    [0024]FIG. 2 is a schematic diagram of atomic clock  10  in accordance with the teachings of the present invention. Cell  12  contains an active medium. For example, cell  12  can contain cesium (Cs) or rubidium (Rb) vapor and buffer gas or gasses. Laser  14  produces optical pumping in cell  12 . Adjustable magnet means  15 ,  16  provides and stabilizes magnetic field B. Photo detector  17  detects laser light transmitted through cell  12 . Alternatively, detection can be through changes in fluorescent emission of the light by the atoms.  
         [0025]    In one embodiment, laser  14  emits circularly polarized D 1  laser light. Laser  14  is modulated simultaneously by modulation frequency intensities generated by harmonic generator  18  and harmonic generator  19 . Harmonic generator  18  is used to generate a frequency v z  of the right Zeeman end resonance. Harmonic generator  19  is used to generate a frequency v m  of the right microwave end resonance. Oscillator  20  can be a small quartz-crystal or other stable local-oscillator “flywheel” providing a frequency v q . A high harmonic of the frequency vq is generated by harmonic generator  18  which is used to generate a microwave end-resonance frequency of the  87 Rb or  133 Cs atoms. A frequency of the corresponding Zeeman end transition from v q  is generated using a low harmonic or a subharmonic of the frequency v q  generated by harmonic or subharmonic generator  19 . The microwave and Zeeman right end resonances share a common sublevel, as shown in FIG. 1. Feedback control loops  21 ,  22  adjust the magnetic field B at cell  12  by controlling adjustable magnet means  15 ,  16  and local-oscillator frequency v q  of oscillator  20  to maximize light reaching photo detector  17 . The frequency of oscillator  20  is always related to the locking frequencies generated by harmonic generator  18  and harmonic generator  19  by preset integer ratios n z  and n m  which are fixed by the design of the harmonic generators  18  and  19 . These two preset, fixed ratios n z =v z /v q  and n m =v m /v q  completely determine the unique values of oscillator frequency v q  and magnetic field B at which the CPT resonance occurs, that is at which the vapor in cell  12  is maximally transparent. Feedback control loop  21  can determine a field error signal from the Zeeman end resonance for control of the magnetic field B. Feedback control loop  22  can determine a frequency error signal from the microwave end resonance for adjusting the frequency v q .  
         [0026]    [0026]FIG. 3 is a flow diagram of a method for operating an atomic clock  30  in accordance with the teachings of the present invention. In block  32 , atoms are optically pumped into a ground-state sublevel having maximum or minimum azimuthal spin angular momentum m. The quantum numbers f and m are used to label the ground-state sublevels of the alkali-metal atom. Here f is the quantum number of the total spin, electronic plus nuclear, of the atom, and m, is the azimuthal quantum number, the projection of the total spin along the direction of the magnetic field. The possible values of f are f=I+½=a or f=I−½=b, and the possible values of m are m=f f−1, f−2, . . . , −f. For example, for a right microwave end resonance, the initial state i, of maximum spin angular momentum has the quantum numbers, f i , m i =a, a. For the same resonance, the corresponding final state j will have the quantum numbers f j , m j =b, b. Most of the atoms can be placed in the initial state by pumping the vapor with circularly polarized light for which the photon spins have one unit of angular momentum parallel to the direction of the magnetic field.  
         [0027]    In block  34 , a microwave end transition and a Zeeman end transition are simultaneously excited with laser light modulated at, or alternating magnetic fields simultaneously oscillating at a microwave frequency of the microwave end resonance and a radio-frequency of the Zeeman end resonance. In block  36 , an applied magnetic field and a local oscillator frequency used for generating the microwave frequency and Zeeman frequency are adjusted in such a way as to maximize the photo detector signal. An embodiment for implementing block  36  is shown in FIG. 7. The end-resonance frequencies can be written as a power series in the magnetic field B. In this embodiment, the expansion is limited to the first power of B and terms of order B 2  are ignored. It will be appreciated that the following description can be used for the exact expression for the frequencies. The present embodiment relates to a clock based on  87 Rb with the nuclear spin quantum number I=3/2. It will be appreciated that the same teachings apply to  133 Cs, having a nuclear spin quantum number of  133 Cs of I=7/2 and twice as many Zeeman sublevels. To first order in B, the frequencies of the left and right Zeeman end resonances are the same and are equal to  
               v   z     =         γ                 B       [   I   ]       .             (   1   )                               
 
         [0028]    The gyromagnetic ratio is  
             γ   =         g                   μ   B       h     =     2.8025                 MHz                     G     -   1       .                 (   2   )                               
 
         [0029]    The Bohr magneton is μ B =9.274×10 −21  erg G −1 , the g factor of the electron is g=2.0023, and Planck&#39;s constant is h=6.626×10 −27  erg sec. The statistical weight of the nuclear spin is denoted [I]=2I+1. For  87 Rb we have I=3/2 and [1]=4, and for  133 Cs, I=7/2 and [1]=8. The magnetic field B will be comparable to the Earth&#39;s field.  
         [0030]    To first order in B, the frequency of the right microwave end resonance is  
               v   m     =       v   hf     +         2      I                 γ                 B       [   I   ]       .               (   3   )                               
 
         [0031]    The hyperfine frequencies are v hf =6834.7 MHz for  87 Rb and v hf =9192.6 MHz for  133 CS. The buffer gas may shift v hf  slightly, and this shift can depend on temperature. The temperature-dependent shifts can be minimized by using an appropriate mixture of gases with positive and negative pressure-shift coefficients, as is currently done with conventional atomic clocks as described in U.S. Pat. No. 2,951,992, hereby incorporated in its entirety into this application.  
         [0032]    The microwave frequency of equation (3) will be much larger than the Zeeman frequency of equation (1). For example, if B=1 G, about twice the ordinary Earth&#39;s field, the following relationship is shown  
                 v   m       v   z       =             [   I   ]          v   hf         γ                 B       +     2      I       =     {             9763.9   +     3                   for   87        Rb                 26264.6   +     7                   for   133        Cs             .                 (   4   )                               
 
         [0033]    From equation (4) it is shown that the resonance frequency of the Zeeman end transition of  87 Rb is about 10,000 smaller than the hyperfine frequency, and the resonance frequency of the Zeeman end transition of  133 CS is about 25,000 smaller than the hyperfine frequency.  
         [0034]    Let the Zeeman resonance frequency be the n z   th  harmonic (or the p z th subharmonic) of the local-oscillator frequency, v q , such that  
                 n   z          v   q       =         γ                 B       [   I   ]       .             (   5   )                               
 
         [0035]    If it is desirable to use a Zeeman frequency lower than the local-oscillator frequency v q , the p z   th  subharmonic can be used, and the frequency relation is  
                   v   q       p   z       =       γ                 B       [   I   ]         ,           (   6   )                               
 
         [0036]    wherein n z  and p z  are positive integers.  
         [0037]    If the microwave resonance frequency v m  is the n m   th  harmonic of the local-oscillator frequency, v q , such that v m =n m v q , it is found that  
                 n   m          v   q       =       v   hf     +         2      I                 γ                 B       [   I   ]       .               (   7   )                               
 
         [0038]    Solving equations (5) and (7) simultaneously, it is found that the ideal frequency of the local-oscillator is  
                 v   qc     =       v   hf         n   m     -     2        In   z             ,           (   8   )                               
 
         [0039]    and the ideal clock frequency is  
               v   c     =         n   m          v   qc       =           n   m          v   hf           n   m     -     2        In   z           .               (   9   )                               
 
         [0040]    The clock frequency of equation (9) is slightly larger (by a ratio of nearly equal, large integers n m  and n m −2In z ) than the zero-field hyperfine frequency v hf  of the atoms.  
         [0041]    The ideal clock field is  
               B   c     =           [   I   ]          n   z          v   qc       γ     =           [   I   ]          n   z          v   hf         γ        (       n   m     -     2        In   z         )         .               (   10   )                               
 
         [0042]    As described above, the field dependence can be eliminated by simply locking the magnetic field to a preset value of equation (10). Accordingly, the field cannot drift and the fact that the microwave end transition is field-dependent does not matter.  
         [0043]    To produce coherent population trapping (CPT) resonances, the vapor can be excited with light which is intensity-modulated at the frequencies of the Zeeman and microwave end resonances. If the two modulation formats are applied simultaneously, the intensity of the incident pumping light is the following  
             I   =             I   0     4     [     1   -     cos        (     2                 π                   n   z          v   q        t     )         ]     [     1   -     cos        (     2                 π                   n   m          v   q        t     )         ]     .             (   11   )                               
 
         [0044]    The sort of time dependence represented by equation (11) is shown in FIG. 4.  
         [0045]    For simplicity, it is assumed that in the vapor the transmittance of light of laser  14 , modulated at a frequency close to the frequency of the Zeeman end resonance is  
               T   z     =       1     1   +     4            (         n   z          v   q       -     γ                   B   /     [   I   ]           )     2     /   Δ                     v   z   2           .             (   12   )                               
 
         [0046]    Here, Δv z  is the full width at half maximum of the Zeeman end resonance, and the transmittance is time-averaged over one Zeeman modulation period.  
         [0047]    In the same vapor, the transmittance of light modulated close to the design frequency of the microwave transition, will be  
                 T   m     =     1     1   +     4            (         n   m          v   q       -     v   hf     -     2      I                 γ                   B   /     [   I   ]           )     2     /   Δ                     v   m   2             ,           (   13   )                               
 
         [0048]    where the full width at half maximum of the microwave end resonance is Δv m .  
         [0049]    Inevitable fluctuations of the magnetic field B and of the local-oscillator frequency v q  can be written as  
           B=B   c   +δB   (14)  
         [0050]    and  
           v   q   =v   qc   +δv   q   (15)  
         [0051]    In terms of these fluctuations, the transmittances of equation (12) and equation (13) become  
                 T   j     =     1     1   +     4                     e   j   2     /   Δ                     v   j   2             ,           (   16   )                               
 
         [0052]    where the resonance index is j=Z orj=m, and the linear combinations e j  of the field and frequency errors are  
               e   z     =           n   z        δ                   v   q       -         γ                 δ                 B       [   I   ]                     and                   e   m         =         n   m        δ                   v   q       -         2      I                 γ                 δ                 B       [   I   ]       .                 (   17   )                               
 
         [0053]    The transmittances of equation (16) are “ridges” that intersect at the origin of the (δB, δv q ) plane, as shown in FIG. 5.  
         [0054]    Feedback control loop  21  and feedback control loop  22  can be used to lock the field B and the local-oscillator frequency v q  to their ideal respective values shown in equation (10) and equation (8). To lock with the end resonances, the field and frequency can be dithered such that  
           B=B   c   +δB+dB  cos Ω B   t   (18)  
         [0055]    and  
           v=v   c   +δv   q   +dv   q  cosΩ v   t   (19)  
         [0056]    This step is shown in block  42  of FIG. 7.  
         [0057]    The dither amplitudes dv q  and dB are chosen to optimize the performance of feedback loop  21  and feedback loop  22 .  
         [0058]    Substituting equations (18) and (19) into equation (16), it is found that  
               T   j     =       1     1   +     4            (       e   j     +     df   j       )     2     /   Δ                     v   j   2           .             (   20   )                               
 
         [0059]    The dither detunings,  
                 df   z     =         n   z          dv   q        cos                   Ω   v        t     -         γ                 d                 B       [   I   ]          cos                   Ω   B        t                 and              
              df   m     =         n   m          dv   q        cos                   Ω   v        t     -         2      I                 γ                 d                 B       [   I   ]          cos                   Ω   B        t         ,             (   21   )                               
 
         [0060]    are quantities fixed by the design of the feedback system. The dither detunings can be chosen to be comparable to, or to be slightly smaller than the resonance linewidths Δv j . The dither frequencies Ω v  and Ω B  are also chosen to be small compared to the natural linewidths Δv j .  
         [0061]    As shown in block  44  of FIG. 7, feedback loop  21  and feedback loop  22  mix the output of photo detector  17  with the fixed dithering frequencies Ω B  and Ω v . The resulting error signals, proportional to the deviations of the clock magnetic field B and local oscillator frequency v q  from their predetermined values B c  and v c  are supplied to magnet control  16  and frequency control  20 .  
         [0062]    Block  46  of FIG. 7 shows that magnet control  16  and frequency control  20  gradually adjust the clock magnetic field B and local oscillator frequency v q  back to their predetermined values given by equations (8) and (9). This action can limit the fluctuations of a resonance variable to values less than the resonance linewidth, divided by the signal-to-noise ratio. Consequently, feedback loop  21  and feedback loop  22  based on the end resonance j, with linewidth Δv j  and signal-to-noise ratio S j  can confine the fluctuations of e to a strip in the (δB; δv q ) plane defined by the two lines  
               e   j     =     ±         Δ                   v   j         S   j       .               (   22   )                               
 
         [0063]    As illustrated in FIG. 5, the Zeeman locking strip of equation (22) with j=z has a width 2Δv z /n z S z  (along the frequency-fluctuation axis) and a slope d(δv q )/d(δB)=γ/n z [I]. The microwave locking strip of equation (22) with j=m has a much smaller width 2Δv m /n m S m  along the frequency fluctuation axis, and it has a much smaller slope d(δv q )/d(δB)=2Iγ/n m [I]. Both the width and the slope of the microwave resonance are much smaller than those of the Zeeman resonance because the harmonic index n m  of the microwave resonance is some four orders of magnitude larger than n z , the harmonic index (or the inverse subharmonic index 1/p z ) of the Zeeman resonance. The fluctuations will be confined to the intersection of these two strips, the parallelogram shown in FIG. 5. From the geometry of FIG. 5 it is shown that the bound on the magnetic field fluctuation is  
               δ                 B     =           [   I   ]                   Δ                   v   z         γ                   S   z         .             (   23   )                               
 
         [0064]    Similarly, the upper right-hand point of the parallelogram in FIG. 5 has a projection on the frequency axis, given by  
               δ                   v   q       =         Δ                   v   m           n   m          S   m         +         2      I                 Δ                   v   z           n   m          S   z         .               (   24   )                               
 
         [0065]    The combined Zeeman and microwave end resonances therefore allow controlling the relative clock frequency to  
                 δ                   v   c         v   c       =           n   m        δ                   v   q         v   hf       =         Δ                   v   m           v   hf          S   m         +         2      I                 Δ                   v   z           v   hf          S   z         .                 (   25   )                               
 
         [0066]    Experiments with end resonances of  87 Rb have demonstrated experimental values Δv m =2 kHz and Δv z =0.8 kHz. With signal acquisition bandwidths of about 1 Hz, and signal-to-noise ratios of S m =S z ≈200, using equation (25) a predicted uncertainty of the clock frequency is  
                 δ                   v   c         v   c       =     2.5   ×       10     -   9       .               (   26   )                               
 
         [0067]    In an alternate embodiment, B is dithered to lock to the Zeeman resonance and v q  is dithered to lock to the microwave resonance. FIG. 6 compares sequential locking trajectories for ridge-climbing dither amplitudes with the scheme where B is dithered to lock to the Zeeman resonance and v q  is dithered to lock to the microwave resonance.  
         [0068]    The present invention can be used for operating an atomic clock or a magnetometer. In the description of the present invention, an ambient magnetic field is the filed produced at the cell  12  by all the objects located outside the embodiment, such as the Earth, the building or the vehicle that the apparatus is in. In the use of a magnetometer, the ambient magnetic field is the field that is measured.  
         [0069]    An adjustable magnetic field is created by means  15 ,  16  in addition to the ambient magnetic field described above in order to stabilize a total magnetic field which is the sum of the ambient magnetic field and the adjustable magnetic field. In use of an atomic clock, the total magnetic field is stabilized to improve the frequency stability of the clock. In use of a magnetometer, the total magnetic field is stabilized such that a measure of the adjustable magnetic field becomes a measure of the ambient magnetic field.  
         [0070]    The “clock field” is the desired value of the ambient magnetic field and the adjustable magnetic field, and the feed-back circuits of the present invention change the adjustable magnetic field in such a way that actual sum of the ambient magnetic field and the adjustable magnetic field does not deviate from the “clock field” by more than is shown by the error parallelograms in FIGS. 5 and 6.  
         [0071]    In one of the embodiments, alternating magnetic fields oscillating at resonance frequencies of the two end resonances are used to excite the resonances. These alternating magnetic fields are the magnetic components of the microwave radiation used in the embodiments. These alternating magnetic fields oscillate so rapidly around their mean zero values that they do not directly contribute to the balance of the ambient magnetic field and the adjustable magnetic field.  
         [0072]    It is to be understood that the above-described embodiments are illustrative of only a few of the many possible specific embodiments which can represent applications of the principles of the invention. Numerous and varied other arrangements can be readily devised in accordance with these principles by those skilled in the art without departing from the spirit and scope of the invention.