Probe beam frequency stabilization in an atomic sensor system

Patent metadata

Field	Value
Publication number	US-10451694-B2
Application number	US-201414188436-A
Country	US
Kind code	B2
Filing date	Feb 24, 2014
Priority date	Feb 24, 2014
Publication date	Oct 22, 2019
Grant date	Oct 22, 2019

Abstract

One example embodiment includes an atomic sensor system. The system includes a vapor cell comprising an alkali metal vapor that precesses in response to a magnetic field. The system also includes a probe laser that generates an optical probe beam that is modulated about a center frequency and which is provided through the vapor cell. A photodetector assembly generates an intensity signal corresponding to a Faraday rotation associated with a detection beam that is associated with the optical probe beam exiting the vapor cell. The system further includes a detection system configured to demodulate the intensity signal at a frequency corresponding to a modulation frequency of the optical probe beam and to generate a feedback signal based on the demodulated intensity signal. The feedback signal is provided to the probe laser to substantially stabilize the center frequency of the optical probe beam based on the feedback signal.

First claim

What is claimed is:

1. An atomic sensor system comprising:
a vapor cell comprising an alkali metal vapor that precesses in response to a magnetic field;
a probe laser configured to generate an optical probe beam that is modulated about a center frequency and which is provided through the vapor cell;
a photodetector assembly configured to generate a first intensity signal corresponding to a Faraday rotation associated with a detection beam that is associated with the optical probe beam exiting the vapor cell, the photodetector assembly comprising:
a polarizing beam-splitter,
a first photodetector, and
a second photodetector,
wherein the polarizing beam-splitter is configured to separate the detection beam into first and second orthogonal polarization signal components,
wherein the first and second photodetectors are configured to generate the first intensity signal and a second intensity signal corresponding to the first and second orthogonal polarization signal components, respectively; and

a detection system comprising:
a summation component configured to add the first and second intensity signals to generate a summation signal, and
a probe controller configured to demodulate the summation signal at a frequency corresponding to a modulation frequency of the optical probe beam and to generate a feedback signal based on the demodulated summation signal that is provided to the probe laser to substantially stabilize the center frequency of the optical probe beam based on the feedback signal.

2. The system of claim 1 , wherein the detection system comprises a difference component configured to subtract the first intensity signal from the second intensity signal to generate a difference signal that corresponds to the Faraday rotation of the detection beam, and wherein the detection system comprises a sensor controller configured to demodulate the difference signal to generate a sensor output signal.

3. The system of claim 1 , wherein the feedback signal is configured to maintain the center frequency of the optical probe beam at a frequency corresponding to a substantial maximum absorption of the optical probe beam by the alkali metal vapor.

4. The system of claim 1 , wherein the optical probe beam is frequency-modulated via a square-wave signal having a positive amplitude and a negative amplitude that are approximately equal and opposite about the center frequency.

5. The system of claim 4 , wherein the positive amplitude of the square-wave signal corresponds to a substantial maximum Faraday rotation associated with the optical probe beam in a first direction and the negative amplitude of the square-wave signal corresponds to a substantial maximum Faraday rotation associated with the optical probe beam in a second direction that is opposite the first direction.

6. The system of claim 1 , wherein the intensity signal comprises a first intensity signal and a second intensity signal that correspond, respectively, to orthogonal polarizations of the optical probe beam, wherein the detection system is configured to demodulate a summation signal corresponding to a sum of the first and second intensity signals to generate the feedback signal.

7. An NMR gyroscope system comprising the atomic sensor system of claim 1 .

8. An atomic magnetometer system comprising the atomic sensor system of claim 1 .

9. A method for stabilizing a frequency of an optical probe beam in an atomic sensor system, the method comprising:
providing the optical probe beam through a vapor cell of the atomic sensor system comprising a precessing alkali metal vapor;
beam-splitting the optical probe beam exiting the vapor cell into orthogonal polarization components;
measuring an intensity of each of the orthogonal polarization components to generate a first intensity signal and a second intensity signal;
adding the first and second intensity signals to generate a summation signal;
generating a feedback signal associated with a magnitude of the summation signal; and
stabilizing the frequency of the optical probe beam based on the feedback signal.

10. The method of claim 9 , further comprising:
modulating the frequency of the optical probe beam about a center frequency based on a modulation signal; and
demodulating the summation signal at a frequency of the modulation signal to generate the feedback signal, wherein stabilizing the frequency of the optical probe beam comprises stabilizing the center frequency of the optical probe beam based on the feedback signal.

11. The method of claim 10 , wherein stabilizing the center frequency of the optical probe beam comprises maintaining the center frequency of the optical probe beam at a frequency corresponding to a substantial maximum absorption of the optical probe beam by the alkali metal vapor.

12. The method of claim 10 , wherein modulating the frequency of the optical probe beam comprises modulating the frequency of the optical probe beam about the center frequency based on the modulation signal configured as a square-wave signal having a positive amplitude and a negative amplitude that are approximately equal and opposite about the center frequency.

13. The method of claim 12 , further comprising:
setting the positive amplitude of the modulation signal to correspond to a first frequency of the optical probe beam associated with a substantial maximum Faraday rotation in a first direction; and setting the negative amplitude of the modulation signal to correspond to a second frequency of the optical probe beam associated with a substantial maximum Faraday rotation in a second direction opposite the first direction.

14. An atomic sensor system comprising:
a vapor cell comprising an alkali metal vapor that precesses in response to a magnetic field;
a probe laser configured to generate an optical probe beam that is modulated about a center frequency via a square-wave modulation signal and which is provided through the vapor cell;
a photodetector assembly configured to generate a first intensity signal and a second intensity signal that correspond, respectively, to orthogonal polarizations of a detection beam corresponding to the optical probe beam exiting the vapor cell; and
a detection system configured to add the first and second intensity signals to generate a summation signal and to demodulate the summation signal at a frequency of the square-wave modulation signal to generate a feedback signal that is provided to the probe laser to substantially stabilize the center frequency of the optical probe beam.

15. The system of claim 14 , wherein the detection system comprises a difference component configured to subtract the first intensity signal from the second intensity signal to generate a difference signal that corresponds to the Faraday rotation of the detection beam, wherein the detection system comprises a sensor controller configured to demodulate the difference signal to generate a sensor output signal.

16. The system of claim 14 , wherein the feedback signal is configured to maintain the center frequency of the optical probe beam at a frequency corresponding to a substantial maximum absorption of the optical probe beam by the alkali metal vapor.

17. The system of claim 14 , wherein the square-wave modulation signal comprises a positive amplitude and a negative amplitude that are approximately equal and opposite about the center frequency.

18. The system of claim 17 , wherein the positive amplitude of the square-wave signal corresponds to a substantial maximum Faraday rotation associated with the optical probe beam in a first d

Assignees

• Bulatowicz Michael D
• Northrop Grumman Systems Corp

Inventors

• Bulatowicz Michael D

Classifications

• G01C19/60

  Electronic or nuclear magnetic resonance gyrometers · CPC title

• G01C19/62

  with optical pumping · CPC title

• G01R33/032

  using magneto-optic devices, e.g. Faraday {or Cotton-Mouton effect} · CPC title

• G01R33/44 Primary

  using nuclear magnetic resonance [NMR] (G01R33/24, G01R33/62 take precedence) · CPC title

• G01R33/26 Primary

  using optical pumping · CPC title