Method and system for pumping of an optical resonator
US-9698558-B2 · Jul 4, 2017 · US
US10199793B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10199793-B2 |
| Application number | US-201715639642-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jun 30, 2017 |
| Priority date | Jul 12, 2013 |
| Publication date | Feb 5, 2019 |
| Grant date | Feb 5, 2019 |
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A method of pumping an optical resonator includes directing light generated by a pumping light at the optical resonator, exciting a propagating surface state of the optical resonator at an interface of the optical resonator, and changing a propagating frequency of the light proximate the interface, where the changed frequency corresponds to a propagation frequency of the surface state. The optical resonator includes a photonic crystal and a material, where the interface is formed between the photonic crystal and the material.
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What is claimed is: 1. A method for pumping an optical resonator, comprising: generating light using a light source; projecting the light at the optical resonator; propagating the light through a photonic crystal such that the light reaches an interface of the optical resonator; changing a frequency of the light near the interface; exciting a surface state of the optical resonator at the interface; and propagating the surface state at the interface. 2. The method of claim 1 , wherein the optical resonator is a spectrally limited optical resonator, wherein the spectrally limited optical resonator is limited in chromatic index. 3. The method of claim 1 , wherein the photonic crystal is one-dimensional, two-dimensional, or three-dimensional. 4. The method of claim 1 , wherein the interface is between the photonic crystal and a metal, a dielectric, another photonic crystal, a gas, air, or vacuum. 5. The method of claim 1 , wherein the surface state includes substantially exponentially functions with a field maximum at the interface. 6. The method of claim 1 , wherein the surface state propagates along the interface after the frequency of the light is changed. 7. The method of claim 1 , wherein the optical resonator includes alternating layers having substantially equal thickness, wherein the photonic crystal includes at least one layer of the alternating layers. 8. A non-transitory computer-readable medium having instructions stored thereon, the instructions forming a program executable by a processing circuit to control pumping an optical resonator, the instructions comprising: instructions to control generation of light using a light source; instructions to control projection of the light at the optical resonator; instructions to excite propagation of the light through a photonic crystal such that the light reaches an interface of the optical resonator; instructions to monitor a change of a frequency of the light near the interface; instructions to monitor excitation of a surface state of the optical resonator at the interface; and instructions to monitor propagation of the surface state at the interface. 9. The non-transitory computer-readable medium of claim 8 , wherein the optical resonator is a spectrally limited optical resonator, wherein the spectrally limited optical resonator is limited in chromatic index. 10. The non-transitory computer-readable medium of claim 8 , wherein the photonic crystal is one-dimensional, two-dimensional, or three-dimensional. 11. The non-transitory computer-readable medium of claim 8 , wherein the interface is between the photonic crystal and a metal, a dielectric, another photonic crystal, a gas, air, or vacuum. 12. The non-transitory computer-readable medium of claim 8 , wherein the surface state includes substantially exponentially functions with a field maximum at the interface. 13. The non-transitory computer-readable medium of claim 8 , wherein the surface state propagates along the interface after the frequency of the light is changed. 14. The non-transitory computer-readable medium of claim 8 , wherein the optical resonator includes alternating layers having substantially equal thickness, wherein the photonic crystal includes at least one layer of the alternating layers. 15. A system for pumping an optical resonator, comprising: a controllable pumping light source configured to: generate light; project the light at the optical resonator, wherein the optical resonator comprises: a photonic crystal; and a material, wherein an interface is formed between the photonic crystal and the material; and a processing circuit configured to: control the generation of the light by the pumping light source; control the direction of the light by the pumping light source; monitor excitation of a propagating surface state of the optical resonator at the interface of the optical resonator; and monitor a change in a propagating frequency of the light at the interface. 16. The system of claim 15 , wherein the optical resonator is a spectrally limited optical resonator, wherein the spectrally limited optical resonator is limited in chromatic index. 17. The system of claim 15 , wherein the photonic crystal is one-dimensional, two-dimensional, or three-dimensional. 18. The system of claim 15 , wherein the material includes a metal, a dielectric, another photonic crystal, a gas, air, or vacuum. 19. The system of claim 15 , wherein the surface state includes substantially exponentially functions with a field maximum at the interface. 20. The system of claim 15 , wherein the surface state propagates along the interface after the frequency of the light is changed.
Construction or shape of the optical resonator {, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region (H01S5/20 takes precedence)} · CPC title
Edge-emitting structures · CPC title
Electricity · mapped topic
in the form of a plate or disc · CPC title
using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering {(mode locking using a non-linear element H01S3/1112)} · CPC title
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