Room-temperature quantum noise limited spectrometry and methods of the same

Patent metadata

Field	Value
Publication number	US-9404801-B2
Application number	US-201414331193-A
Country	US
Kind code	B2
Filing date	Jul 14, 2014
Priority date	Mar 30, 2010
Publication date	Aug 2, 2016
Grant date	Aug 2, 2016

Abstract

In one embodiment, a heterodyne detection system for detecting light includes a first input aperture configured to receive first light from a scene input, a second input aperture configured to receive second light from a local oscillator input, a broadband local oscillator configured to provide the second light to the second input aperture, a dispersive element configured to disperse the first light and the second light, and a final condensing lens coupled to an infrared detector. The final condensing lens is configured to concentrate incident light from a primary condensing lens onto the infrared detector, and the infrared detector is a square-law detector capable of sensing the frequency difference between the first light and the second light. More systems and methods for detecting light are described according to other embodiments.

First claim

What is claimed is:

1. A heterodyne detection system for detecting light, comprising:
a first input aperture configured to receive first light from a scene input;
a second input aperture configured to receive second light from a local oscillator input;
a broadband local oscillator configured to provide the second light to the second input aperture;
a dispersive element configured to disperse the first light and the second light; and
a final condensing lens coupled to an infrared detector,
wherein the final condensing lens is configured to concentrate incident light from a primary condensing lens onto the infrared detector,
wherein the infrared detector is a square-law detector configured to sense a frequency difference between the first light and the second light; and
wherein each area of the first and second input apertures times an input collection solid angle of the system is about a wavelength squared (about λ 2 ).

2. The heterodyne detection system as recited in claim 1 , further comprising a radio frequency (RF) waveguide, wherein the RF waveguide is configured to facilitate optical upconversion of RF energy generated by the infrared detector.

3. The heterodyne detection system as recited in claim 1 , wherein at each detector pixel, a frequency of light from the scene input and a frequency of light from the oscillator input coincide with a bandwidth determined by a spectral resolution of the system, and
wherein the detection system is configured such that the two frequencies create a coherent beat frequency.

4. The heterodyne detection system as recited in claim 1 , further comprising a radio frequency (RF) waveguide, wherein the RF waveguide is coplanar to the infrared detector.

5. The heterodyne detection system as recited in claim 1 , wherein the infrared detector comprises:
a photodetector element; and
an RF detector element decoupled from the photodetector element.

6. The heterodyne detection system as recited in claim 5 , wherein the photodetector element comprises a quantum well infrared photodetector (QWIP), and wherein the RF detector element comprises a carbon nanotube antenna.

7. The heterodyne detection system as recited in claim 1 , wherein the broadband local oscillator comprises a broadband quantum cascade laser having broad spectral bands between about 500 cm −1 and about 5000 cm −1 .

8. The heterodyne detection system as recited in claim 1 , wherein the first input aperture is spatially offset from the second input aperture, wherein the first and second light pass through the first and second apertures in a same direction relative to each other.

9. A heterodyne detection system for detecting light, comprising:
a first input aperture configured to receive first light from a scene input;
a second input aperture configured to receive second light from a local oscillator input;
a broadband local oscillator configured to provide the second light to the second input aperture;
a dispersive element configured to disperse the first light and the second light; and
a final condensing lens coupled to an infrared detector;
wherein the final condensing lens is configured to concentrate incident light from a primary condensing lens onto the infrared detector;
wherein the infrared detector is a square-law detector configured to sense a frequency difference between the first light and the second light;
wherein the final condensing lens comprises a plasmonic infrared (IR) condensing lens;
wherein the plasmonic IR condensing lens has a conical shape tapering inward toward the infrared detector, and comprises a Si core having a conductive metal cladding on radial surfaces thereof; and
wherein the conical shape has a first diameter at an end adjacent the infrared detector of less than about one-half wavelength of the incident light in Si, and wherein the conical shape has a second diameter at an end receiving the incident light from the dispersive element of approximately a diffraction limit set by the primary condensing lens.

10. A method for detecting light, the method comprising:
receiving first light from a desired scene in a first input aperture of a spectrometer;
introducing second light produced by a broadband local oscillator to a second input aperture;
passing the first light from the desired scene and the second light produced by the broadband local oscillator through a dispersive element;
concentrating the light from the dispersive element onto a detector pixel of an infrared detector using a condensing lens coupled to the infrared detector; and
detecting simultaneously the first light and the second light using the infrared detector,
wherein the concentrating reduces an intrinsic detector noise resulting from dark current by a factor of at least 20.

11. The method as recited in claim 10 , further comprising:
generating radio-frequency (RF) energy using the infrared detector in response to detecting the first light and the second light; and
optically upconverting the generated RF energy.

12. The method as recited in claim 11 , further comprising creating a coherent beat frequency using the two frequencies, wherein each area of the first and second input apertures times a collection solid angle of the spectrometer is about a wavelength squared (about λ 2 ).

13. The method as recited in claim 11 , wherein the upconverting comprises:
channeling the generated RF energy to a close-coupled RF waveguide; and
interacting the channeled RF energy with a laser beam, wherein the interacting generates an optical electric field.

14. The method as recited in claim 13 , wherein the interacting is performed at an electro-optic modulator coupled to an RF waveguide.

15. The method as recited in claim 10 , wherein the broadband local oscillator comprises a broadband quantum cascade laser having broad spectral bands between about 500 cm −1 and about 5000 cm −1 .

16. The method as recited in claim 10 , wherein the first input aperture is spatially offset from the second input aperture, and
wherein the first and second light pass through the first and second apertures in a same direction relative to each other.

17. The method as recited in claim 10 , wherein the condensing lens comprises a plasmonic infrared (IR) condensing lens.

Assignees

• L Livermore Nat Security Llc

Inventors

• Stevens Charles G
• Tringe Joseph W
• Cunningham christopher t

Classifications

• G01J3/453 Primary

  by correlation of the amplitudes · CPC title

• G01J3/10

  Arrangements of light sources specially adapted for spectrometry or colorimetry · CPC title

• G01J3/4338

  Frequency modulated spectrometry · CPC title

• G01N21/35

  using infrared light (G01N21/39 takes precedence) · CPC title