Integrated devices for squeezed light generation

1. An apparatus, comprising:

an optical medium characterized by a third-order nonlinear optical susceptibility, the optical medium including a first ring resonator;

a pump light source in optical communication with the optical medium and configured to send a pump light beam to the optical medium, the pump light beam including a pulsed light beam;

a drive light source in optical communication with the optical medium and configured to send a drive light beam to the optical medium, the drive light beam including a continuous wave (CW) light beam, the pump light beam and the drive light beam being configured to generate a signal light beam in a squeezed state of light via spontaneous four-wave mixing in the optical medium,

a coupler in optical communication with the first ring resonator and configured to couple the pump light beam and the drive light beam into the first ring resonator; and

a second ring resonator in optical communication with the first ring resonator and configured to suppress auxiliary resonance within the first ring resonator.

2. The apparatus of claim 1 , wherein the optical medium includes silicon nitride.

3. The apparatus of claim 1 , wherein the coupler includes:

a Mach-Zehnder interferometer (MZI) in optical communication with the first ring resonator and configured to couple the pump light beam and the drive light beam into the first ring resonator.

4. The apparatus of claim 1 , wherein coupler includes:

a racetrack coupler in optical communication with the first ring resonator and configured to couple the pump light beam and the drive light beam into the first ring resonator.

5. The apparatus of claim 1 , wherein the drive light beam is configured to drive the spontaneous four-wave mixing and detune a resonance frequency of the pump light beam and a resonance frequency of the signal light beam.

6. The apparatus of claim 1 , wherein the pump light beam is configured to generate the signal light beam in a single-temporal-mode squeezed vacuum state.

7. The apparatus of claim 1 , wherein a first power of the pump light beam is less than 10% of a second power of the drive light beam so as to decrease an effect of dynamical self-phase modulation and an effect of dynamical cross-phase modulation induced by the pump light beam.

8. An apparatus, comprising:

an optical medium characterized by a third-order nonlinear optical susceptibility, the optical medium including a ring resonator;

a pump light source in optical communication with the optical medium and configured to send a pump light beam to the optical medium, the pump light beam including a pulsed light beam;

a drive light source in optical communication with the optical medium and configured to send a drive light beam to the optical medium, the drive light beam including a continuous wave (CW) light beam, the pump light beam and the drive light beam being configured to generate a signal light beam in a squeezed state of light via spontaneous four-wave mixing in the optical medium;

a first coupler in optical communication with the ring resonator and configured to couple the pump light beam and the drive light beam into the ring resonator; and

a second coupler in optical communication with the ring resonator and configured to suppress auxiliary resonance within the ring resonator.

9. A method, comprising:

sending, via a coupler, a pump light beam into an optical medium characterized by a third-order nonlinear optical susceptibility, the pump light beam including a pulsed light beam and the optical medium including a first ring resonator;

coupling a drive light beam into the optical medium via the coupler to interact with the pump light beam so as to generate a signal light beam at a squeezed state of light via spontaneous four-wave mixing in the optical medium, the drive light beam including a continuous wave (CW) light beam;

suppressing auxiliary resonances within the first ring resonator using a second ring resonator disposed in optical communication with the first ring resonator.

10. The method of claim 9 , further comprising:

adjusting a power of at least one of the pump light beam or the drive light beam so as to change a squeezing factor of the squeezed state of light.

11. The method of claim 9 , further comprising:

adjusting a phase of at least one of the pump light beam or the drive light beam so as to change a phase of the squeezed state of light.

12. The method of claim 9 , further comprising:

adjusting a frequency of at least one of the pump light beam or the drive light beam so as to change a squeezing factor of the squeezed state of light.

13. The method of claim 9 , wherein sending the pump light beam includes sending the pump light beam into silicon nitride.

14. The method of claim 9 , further comprising:

adjusting a first coupling between the pump light beam and the first ring resonator using a Mach-Zehnder interferometer (MZI) configured to couple the pump light beam into the first ring resonator; and

adjusting a second coupling between the drive light beam and the first ring resonator using the MZI.

15. The method of claim 9 , further comprising:

adjusting a first coupling between the pump light beam and the first ring resonator using a racetrack coupler configured to couple the pump light beam into the first ring resonator; and

adjusting a second coupling between the drive light beam and the first ring resonator using the racetrack coupler.

16. The method of claim 9 , wherein sending the drive light beam includes sending the drive light beam having a power to drive the spontaneous four-wave mixing within the optical medium and detune a resonance frequency of the pump light beam and a resonance frequency of the signal light beam.

17. The method of claim 9 , wherein sending the pump light beam includes sending the pump beam to generate the signal light beam in a single-temporal-mode squeezed vacuum state.

18. The method of claim 9 , further comprising:

decreasing a power of the pump light beam so as to decrease an effect of self-phase modulation and an effect of cross-phase modulation induced by the pump light beam.

19. A method, comprising:

sending a pump light beam into an optical medium characterized by a third-order nonlinear optical susceptibility, the pump light beam including a pulsed light beam and the optical medium including a ring resonator;

sending a drive light beam into the optical medium to interact with the pump light beam so as to generate a signal light beam at a squeezed state of light via spontaneous four-wave mixing in the optical medium, the drive light beam including a continuous wave (CW) light beam; and

suppressing auxiliary resonances within the ring resonator using an auxiliary coupler disposed in optical communication with the ring resonator.

20. A system, comprising:

a ring resonator including an optical medium characterized by a third-order nonlinear optical susceptibility;

a linear waveguide in optical communication with the ring resonator and configured to propagate a pump light beam and a drive light beam;

a first coupler in optical communication with the ring resonator and the linear waveguide and configured to couple the pump light beam and the drive light beam into the ring resonator, the drive light beam and pump light beam being configured to reduce an effect of time-varying self-phase modulation and an effect of time-varying cross-phase modulation, the pump light beam and the drive light beam being further configured to generate a signal light beam in a squeezed light of state via four-wave mixing; and

a second coupler in optical communication with the ring resonator and configured to suppress auxiliary resonances within the ring resonator.