Atomic magnetometer
An atomic magnetometer system includes a laser system, a cell, and an optics setup. The laser system is configured to generate a pump beam and a probe beam. The cell encloses an atomic vapor. The optics setup is configured to route the pump beam and the probe beam. The pump beam propagates along a path through the atomic vapor and the probe beam also propagates substantially along the path through the atomic vapor. The pump beam and the probe beam traverse the atomic vapor along two or more non-parallel directions. The interaction of the pump beam with the atomic vapor is modulated at or near harmonics of a magnetic resonance frequency.
1. An atomic magnetometer system, comprising:
a laser system configured to generate a pump beam and a probe beam;
a cell enclosing an atomic vapor;
an optics setup configured to route the pump beam and the probe beam, wherein the pump beam propagates along a path through the atomic vapor and the probe beam also propagates substantially along the path through the atomic vapor,
wherein the pump beam and the probe beam enter the atomic vapor along a first direction, and
wherein the pump beam and the probe beam traverse the atomic vapor along a second direction, wherein the first direction and the second direction are non-parallel directions,
wherein an interaction of the pump beam with the atomic vapor is modulated at harmonics of a magnetic resonance frequency.
2. The atomic magnetometer system as in claim 1 , wherein the pump beam is amplitude modulated.
3. The atomic magnetometer system as in claim 1 , wherein the pump beam is frequency modulated.
4. The atomic magnetometer system as in claim 1 , wherein the probe beam is not modulated at or near the magnetic resonance frequency.
5. The atomic magnetometer system as in claim 1 , wherein the probe beam is linearly polarized.
6. The atomic magnetometer system as in claim 1 , wherein the probe beam is circularly polarized.
7. The atomic magnetometer system as in claim 1 , wherein a polarization of the probe beam is resolved after the atomic vapor and optical rotation or induced ellipticity is measured to detect spin precession within the atomic vapor.
8. The atomic magnetometer system as in claim 1 , wherein a power of the probe beam is measured after the atomic vapor and a probe beam's absorption is used to detect spin precession within the atomic vapor.
9. The atomic magnetometer system as in claim 1 , wherein the pump beam and the probe beam are generated by different lasers.
10. The atomic magnetometer system as in claim 9 , wherein the pump beam and the probe beam are tuned to two substantially different wavelengths, each of which is near an optical transition of an alkali vapor.
11. The atomic magnetometer system as in claim 10 , wherein the pump beam is blocked after traversing the cell enclosing the atomic vapor by an interference filter.
12. The atomic magnetometer system as in claim 1 , wherein the pump beam and the probe beam are generated by a common laser.
13. The atomic magnetometer system as in claim 12 , wherein the common laser is sequentially tuned in wavelength and/or power to achieve pumping and probing of the alkali atomic vapor at different times.
14. The atomic magnetometer system as in claim 12 , wherein a polarization-tuning element changes a polarization of an output of the common laser to achieve pumping and probing of the atomic vapor at different times.
15. The system as in claim 1 , wherein the atomic magnetometer system comprises a scalar magnetometer.
16. The atomic magnetometer system as in claim 15 , wherein the atomic magnetometer system operates in a finite nonzero magnetic field.
17. The atomic magnetometer system as in claim 15 , wherein the atomic magnetometer system operates with a spin-precession frequency that is larger than a spin relaxation rate.
18. The atomic magnetometer system as in claim 1 , wherein an optic expands or focuses the pump beam and the probe beam to cause each of them to span multiple propagation directions.
19. The atomic magnetometer system as in claim 18 , wherein a path of a converging beam or a diverging beam generated by the pump beam and the probe beam can be described as having a cone shape or a conical surface.
20. The atomic magnetometer system as in claim 19 , wherein a half opening angle of the cone shape is approximately equal to 54.7356°.
21. A method for an atomic magnetometer system, comprising:
providing a laser configured to generate a pump beam and a probe beam;
providing a cell enclosing an atomic vapor; and
providing an optics setup configured to route the pump beam and the probe beam, wherein the pump beam and the probe beam co-propagate through the atomic vapor, wherein the pump beam and the probe beam enter the atomic vapor along a first direction and wherein pump beam and the probe beam traverse the atomic vapor along a second direction, wherein the first direction and the second direction are non-parallel directions.