Quasi-linear spin torque nano-oscillators
US-2015372687-A1 · Dec 24, 2015 · US
US9444476B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9444476-B2 |
| Application number | US-201314420709-A |
| Country | US |
| Kind code | B2 |
| Filing date | Aug 28, 2013 |
| Priority date | Aug 30, 2012 |
| Publication date | Sep 13, 2016 |
| Grant date | Sep 13, 2016 |
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An atomic oscillator includes an alkali-metal cell in which alkali-metal atoms are enclosed, a light source which irradiates the atoms in the alkali-metal cell with laser beams, a photodetector which detects a light amount of the laser beams passing through the alkali-metal cell to enter the photodetector, and a controller which generates sidebands including a pair of laser beams with different wavelengths by performing frequency modulation of a carrier on the light source, causes the pair of laser beams with the different wavelengths to enter the alkali-metal cell, and controls a modulation frequency according to optical absorption characteristics of the atoms by quantum interference effects of a pair of resonance laser beams, wherein the side bands include second-order or higher-order sidebands.
Opening claim text (preview).
The invention claimed is: 1. An atomic oscillator comprising: an alkali-metal cell in which alkali-metal atoms are enclosed; a light source configured to irradiate the atoms in the alkali-metal cell with laser beams; a photodetector configured to detect a light amount of the laser beams passing through the alkali-metal cell to enter the photodetector; a controller configured to generate a pair of laser beams with different wavelengths by performing frequency modulation of a carrier on the light source, cause the pair of laser beams with the different wavelengths to enter the alkali-metal cell, and control a modulation frequency according to optical absorption characteristics of the atoms by quantum interference effects of a pair of resonance laser beams, wherein the laser beams entering the alkali-metal cell are pulsed laser beams; and a detector configured to detect a Ramsey interrogation signal, in a pulsed interrogation mode, wherein the pair of laser beams with the different wavelengths are both third-order sidebands, to permit the modulation frequency for the Ramsey interrogation signal to be reduced. 2. The atomic oscillator according to claim 1 , wherein the pulsed laser beams have a waveform in a form of a square wave. 3. The atomic oscillator according to claim 1 , wherein the pulsed laser beams have a waveform in a form of a triangular wave. 4. The atomic oscillator according to claim 1 , wherein the controller is configured to generate the pulsed laser beams by modulating the laser beams emitted from the light source by using a liquid crystal element. 5. The atomic oscillator according to claim 1 , wherein the light source is made of a surface emitting laser. 6. An interrogation method of CPT resonance by an atomic oscillator including an alkali-metal cell in which alkali-metal atoms are enclosed, a light source configured to irradiate the atoms in the alkali-metal cell with laser beams, and a photodetector configured to detect a light amount of the laser beams passing through the alkali-metal cell to enter the photodetector, the interrogation method comprising: generating a pair of laser beams with different wavelengths by performing frequency modulation of a carrier on the light source; causing the pair of laser beams with the different wavelengths to enter the alkali-metal cell, wherein the laser beams entering the alkali-metal cell are pulsed laser beams; detecting a Ramsey interrogation signal, in a pulsed interrogation mode; and controlling a modulation frequency according to optical absorption characteristics of the atoms by quantum interference effects of a pair of resonance laser beams, wherein the pair of laser beams with the different wavelengths are both third-order sidebands, to permit the modulation frequency for the Ramsey interrogation signal to be reduced. 7. The interrogation method according to claim 6 , wherein the pulsed laser beams have a waveform in a form of a square wave. 8. The interrogation method according to claim 6 , wherein the pulsed laser beams have a waveform in a form of a triangular wave. 9. The interrogation method according to claim 6 , wherein the generating includes generating the pulsed laser beams by modulating the laser beams emitted from the light source by using a liquid crystal element. 10. The interrogation method according to claim 6 , wherein the light source is made of a surface emitting laser.
Generation of oscillations using radiation source and detector, e.g. with interposed variable obturator · CPC title
Stabilising the frequency of the laser · CPC title
using energy levels of molecules, atoms, or subatomic particles as a frequency reference · CPC title
for modulating the output, i.e. the laser beam is modulated outside the laser cavity · CPC title
using Coherent Population Trapping · CPC title
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