Pulsed free induction decay nonlinear magneto-optical rotation apparatus
A magnetometer and concomitant magnetometry method comprising emitting light from a light source, via a pulse generator pulsing light from the light source, directing the pulsed light to an atomic chamber, employing a field sensor in the atomic chamber, and via a signal processing module receiving a signal from the field sensor.
1. A magnetometer comprising:
a light source;
a pulse generator permitting pulsing of light from said light source;
a path for the pulsed light to travel to an atomic chamber;
a field sensor in said atomic chamber; and
a signal processing module receiving a signal from said field sensor; and
wherein said magnetometer does not employ a means for applying a magnetic field to said atomic chamber.
2. The magnetometer of claim 1 wherein said pulsed light is linearly polarized.
3. The magnetometer of claim 1 wherein said field sensor comprises an atomic vapor selected from the group consisting of lithium, sodium, rubidium, and cesium.
4. The magnetometer of claim 1 wherein said light source is a dye laser.
5. The magnetometer of claim 1 wherein said light source is a diode laser.
6. The magnetometer of claim 1 wherein said light source is a distributed feedback laser.
7. The magnetometer of claim 1 wherein said light source is a vertical cavity surface emitting laser.
8. The magnetometer of claim 1 wherein said path is a single path.
9. The magnetometer of claim 1 wherein said pulsed light is amplitude, frequency, or wavelength modulated.
10. The magnetometer of claim 1 wherein said pulse generator uses a pulse duration shorter than approximately ¼ of the Larmor precession period of atoms in said atomic chamber.
11. The magnetometer of claim 10 wherein said pulse generator produces a succession of pulses during a pump period, the time between pulses being about equal to ½ the Larmor precession period or integer multiples thereof.
12. The magnetometer of claim 1 wherein said pulse generator produces a succession of one or more pulses during a pump period and is operated at a stable level during a probe period.
13. The magnetometer of claim 1 wherein said signal processing module comprises a balanced polarimeter, two photodetectors, and a difference amplifier.
14. The magnetometer of claim 1 wherein said signal processing module comprises a nearly crossed polarimeter and a single photodetector.
15. The magnetometer of claim 1 wherein said signal processing module comprises a sensor of fluorescence from said field sensor.
16. The magnetometer of claim 1 wherein said signal processing module employs a probe beam.
17. The magnetometer of claim 16 wherein said signal processing module employs a linearly polarized probe beam.
18. A magnetometry method comprising the steps of:
emitting light from a light source;
via a pulse generator, pulsing light from the light source;
directing the pulsed light to an atomic chamber;
employing a field sensor in the atomic chamber; and
via a signal processing module, receiving a signal from the field sensor; and
wherein the method does not apply a magnetic field to the atomic chamber.
19. The method of claim 18 additionally comprising the step of linearly polarizing the pulsed light.
20. The method of claim 18 wherein the field sensor comprises an atomic vapor selected from the group consisting of lithium, sodium, rubidium, and cesium.
21. The method of claim 18 wherein the light source is a dye laser.
22. The method of claim 18 wherein the light source is a diode laser.
23. The method of claim 18 wherein the light source is a distributed feedback laser.
24. The method of claim 18 wherein the light source is a vertical cavity surface emitting laser.
25. The method of claim 18 wherein the directing step employs a single path.
26. The method of claim 18 additionally comprising the step of amplitude, frequency, or wavelength modulating the pulsed light.
27. The method of claim 18 wherein the pulse generator uses a pulse duration shorter than approximately ¼ of the Larmor precession period of atoms in the atomic chamber.
28. The method of claim 27 wherein the pulse generator produces a succession of pulses during a pump period, the time between pulses being about equal to ½ the Larmor precession period or integer multiples thereof.
29. The method of claim 18 wherein the pulse generator produces a succession of one or more pulses during a pump period and is operated at a stable level during a probe period.
30. The method of claim 18 wherein the signal processing module comprises a balanced polarimeter, two photodetectors, and a difference amplifier.
31. The method of claim 18 wherein the signal processing module comprises a nearly crossed polarimeter and a single photodetector.
32. The method of claim 18 wherein the signal processing module comprises a sensor of fluorescence from the field sensor.
33. The method of claim 18 wherein the signal processing module employs a probe beam.
34. The method of claim 33 wherein the signal processing module employs a linearly polarized probe beam.
35. A magnetometer comprising:
a pulsed light source;
a continuous-wave light source;
a pulse generator permitting pulsing of light from said pulsed light source;
a path for said pulsed light to travel to an atomic chamber;
a path for said continuous-wave light to travel to said atomic chamber;
a field sensor generating an optical signal in said atomic chamber;
a signal processing module receiving said optical signal from said field sensor; and
a path for said optical signal to travel to said signal processing modulei and
wherein said magnetometer does not employ a means for applying a magnetic field to said atomic chamber.