System and method for nonlinear optical devices

• US 9,000,347 B2
• Filed: 10/05/2012
• Issued: 04/07/2015
• Est. Priority Date: 10/05/2011
• Status: Active Grant

• Current Assignee: Telcordia Technologies Incorporated (Telefonaktiebolaget LM Ericsson)
• Original Assignee: Telcordia Technologies Incorporated (Telefonaktiebolaget LM Ericsson)
• Inventors: Woodward, Ted, Agarwal, Anjali, Peters, Nicholas
• Primary Examiner(s): Ko, Tony
• Application Number:
  US13/646,435
• Publication Number:
  US 20130087689A1
• Time in Patent Office: 914 Days
• Field of Search: 250/208.1, 250/214.1, 250/214.R
• US Class Current: 250/214.R
• CPC Class Codes: G01J 1/0425 using optical fibers
• CPC Class Codes: G01J 1/0459 using an optical amplifier of light or coatings to improve optical coupling
• CPC Class Codes: G01J 1/42 using electric radiation detectors optical or mechanical part G01J1/04; by comparison with a reference light or electric value G01J1/10
• CPC Class Codes: G01J 1/58 using luminescence generated by light
• CPC Class Codes: G01J 3/4531 Devices without moving parts
• CPC Class Codes: G01N 21/17 Systems in which incident light is modified in accordance with the properties of the material investigated where the material investigated is optically excited causing a change in wavelength of the incident light G01N21/63
• CPC Class Codes: G01N 21/41 Refractivity; Phase-affecting properties, e.g. optical path length G01N21/21 takes precedence
• CPC Class Codes: G01S 17/10 using transmission of interrupted, pulse-modulated waves determination of distance by phase measurements G01S17/32
• CPC Class Codes: G01S 7/486 Receivers
• CPC Class Codes: G01S 7/487 Extracting wanted echo signals , e.g. pulse detection
• CPC Class Codes: G02B 6/29338 Loop resonators
• CPC Class Codes: G02F 1/3536 Four-wave interaction
• CPC Class Codes: G02F 1/39 for parametric generation or amplification of light, infrared or ultraviolet waves
• CPC Class Codes: G02F 1/392 Parametric amplification
• CPC Class Codes: H01L 31/0232 Optical elements or arrangements associated with the device H01L31/0236 takes precedence; for photovoltaic cells H01L31/054; for photovoltaic modules H02S40/20
• CPC Class Codes: H04B 10/70 Photonic quantum communication

Abstract

Systems for enhancing the sensitivity of detecting an optical signal using nonlinear optics and method of performing the same. In one embodiment, a single-photon detection system includes an optical amplifier realized in a waveguide, and a photodetector coupled to an output of the optical amplifier. A light detection and ranging system includes the optical amplifier coupled to an optical source and one photodetector. In another embodiment, a photodetection system includes a plurality of optical frequency converters, coupled to an optical source, that sequentially convert a wavelength of photons of the optical source to a final wavelength, and a single-photon photodetector coupled to the optical frequency converters to detect single photons produced by the optical source. In another embodiment, an optical sensor includes an optical pump, and a transducer including an optical ring cavity coupled to the optical pump and configured to utilize optical four-wave mixing to detect an external stimulus.

Claims

1. A photodetection system, comprising:

a cascaded plurality of optical frequency converters coupled to an optical source, each of said plurality of optical frequency converters being configured to sequentially convert a wavelength of photons of said optical source to a final wavelength; and

a single-photon photodetector coupled to said plurality of optical frequency converters to detect single photons produced by said optical source.

2. The photodetection system as recited in claim 1 wherein said plurality of cascaded optical frequency converters are configured to produce photons with wavelengths lying in a monotonic sequence from said wavelength of photons produced by said optical source to a wavelength of a final one of said plurality of optical frequency converters.

3. The photodetection system as recited in claim 1 wherein each of said plurality of optical frequency converters are configured to utilize an optical four-wave mixing process.

4. The photodetection system as recited in claim 1 wherein each of said plurality optical frequency converters are configured to utilize Chi(3) nonlinear optical interactions.

5. The photodetection system as recited in claim 1 wherein said plurality of optical frequency converters are configured to utilize a combination of Chi(2) and Chi(3) nonlinear optical interactions.

6. The photodetection system as recited in claim 1 wherein an optical input signal produced by said optical source has a mean photon number less than one.

7. The photodetection system as recited in claim 1 further comprising a plurality of pumps configured to provide pump inputs to respective ones of said plurality of optical frequency converters.

8. The photodetection system as recited in claim 7 wherein each of said plurality of pumps comprise a laser having a selected wavelength.

9. The photodetection system as recited in claim 7 wherein each of said plurality of pumps comprise a continuous wave laser pump with a maximum power greater than or equal to one watt.

10. The photodetection system as recited in claim 1 wherein said single-photon photodetector is a silicon avalanche photodiode single-photon detector.

11. A method of operating a photodetection system, comprising:

coupling a cascaded plurality of optical frequency converters to an optical source, each of said plurality of optical frequency converters being configured to sequentially convert a wavelength of photons of said optical source to a final wavelength; and

coupling a single-photon photodetector to said plurality of optical frequency converters to detect single photons produced by said optical source.

12. The method as recited in claim 11 wherein said plurality of cascaded optical frequency converters are configured to produce photons with wavelengths lying in a monotonic sequence from said wavelength of photons produced by said optical source to a wavelength of a final one of said plurality of optical frequency converters.

13. The method as recited in claim 11 wherein each of said plurality of optical frequency converters are configured to utilize an optical four-wave mixing process.

14. The method as recited in claim 11 wherein each of said plurality optical frequency converters are configured to utilize Chi(3) nonlinear optical interactions.

15. The method as recited in claim 11 wherein said plurality of optical frequency converters are configured to utilize a combination of Chi(2) and Chi(3) nonlinear optical interactions.

16. The method as recited in claim 11 wherein an optical input signal produced by said optical source has a mean photon number less than one.

17. The method as recited in claim 11 further comprising providing a plurality of pumps configured to provide pump inputs to respective ones of said plurality of optical frequency converters.

18. The method as recited in claim 17 wherein each of said plurality of pumps comprise a laser having a selected wavelength.

19. The method as recited in claim 17 wherein each of said plurality of pumps comprise a continuous wave laser pump with a maximum power greater than or equal to one watt.

20. The method as recited in claim 11 wherein said single-photon photodetector is a silicon avalanche photodiode single-photon detector.