Devices, compositions and methods for imaging with raman scattering
US-2016243261-A1 · Aug 25, 2016 · US
US9830555B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9830555-B2 |
| Application number | US-201414904040-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 9, 2014 |
| Priority date | Jul 9, 2013 |
| Publication date | Nov 28, 2017 |
| Grant date | Nov 28, 2017 |
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In one aspect, a computational machine includes an optical device configured to receive energy from an optical energy source and generate a number N 1 of optical signals, and a number N 2 of coupling devices, each of which controllably couples a plurality of the number N 1 optical signals. The coupling devices are individually controlled to simulate a computational problem. In another aspect, a computational machine includes a number N 1 of parametric oscillators and a number N 2 of coupling devices, each of which controllably couples a plurality of the number N 1 of parametric oscillators together. The coupling devices are individually controlled to simulate a computational problem.
Opening claim text (preview).
The invention claimed is: 1. A computational machine, comprising: an optical device configured to receive energy from an optical energy source and generate a number N 1 of optical signals, N 1 is 2 or greater; and a number N 2 of coupling devices, each of which controllably couples a plurality of the number N 1 of optical signals, N 2 is 1 or greater; wherein the coupling devices are individually controlled to simulate a computational problem. 2. The computational machine of claim 1 , wherein the optical energy source is a laser. 3. The computational machine of claim 1 , further comprising a controller configured to control the optical energy source to produce energy in a predefined pattern. 4. The computational machine of claim 1 , wherein the number N 2 is equal to one half of the value N 1 squared minus N 1 (N 2 =(N 1 ^2−N 1 )/2. 5. The computational machine of claim 1 , wherein the number N 2 is equal to the value N 1 minus one (N 2 =N 1 −1). 6. The computational machine of claim 1 , wherein the number N 2 is equal to one (N 2 =1). 7. The computational machine of claim 1 , wherein the N 1 optical signals are generated from a plurality of optical parametric oscillators (OPOs). 8. The computational machine of claim 7 , wherein the OPOs are implemented using microresonators. 9. The computational machine of claim 1 , configured to produce and maintain the N 1 optical signals within one resonant cavity or one optical fiber. 10. The computational machine of claim 1 , wherein the coupling devices include electro-optic modulators (EOMs). 11. The computational machine of claim 1 , wherein the computational problem is one of a nondeterministic polynomial (NP) problem, an Ising problem, or an optimization problem. 12. The computational machine of claim 1 , configured to produce a set of numbers from a plurality of the N 1 signals, wherein the produced numbers contain information about a solution of the computational problem. 13. The computational machine of claim 12 , wherein the produced numbers determine a solution to the computational problem. 14. The computational machine of claim 12 , wherein the produced numbers are generated from the phases of a plurality of the N 1 signals. 15. The computational machine of claim 12 configured to provide a phase reference, wherein at least one of the N 1 optical signals is compared to the phase reference to produce the numbers. 16. The computational machine of claim 12 , wherein at least two of the N 1 signals are compared to each other to produce the numbers. 17. A computational machine, comprising: a number N 1 of parametric oscillators, N 1 is 2 or greater; and a number N 2 of coupling devices, each of which controllably couples a plurality of the number N 1 of parametric oscillators together, N 2 is 1 or greater; wherein the coupling devices are individually controlled to simulate a computational problem. 18. The computational machine of claim 17 , wherein the parametric oscillators are optical parametric oscillators. 19. The computational machine of claim 18 , wherein the optical parametric oscillators are selected from continuous wave degenerate optical parametric oscillators and pulsed degenerate optical parametric oscillators. 20. The computational machine of claim 17 , wherein the parametric oscillators are time-multiplexed in one optical cavity or optical fiber.
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