Terahertz radiator based on coherent SPR amplified by stimulation
US-12149041-B2 · Nov 19, 2024 · US
US9966720B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9966720-B2 |
| Application number | US-201615261300-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 9, 2016 |
| Priority date | Sep 10, 2015 |
| Publication date | May 8, 2018 |
| Grant date | May 8, 2018 |
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Masers and microwave amplifiers that can function in the continuous-wave mode at room temperature are provided. The maser system can include a diamond gain medium having nitrogen-vacancy centers, and a resonator can be disposed around the gain medium. The resonator can be disposed in a cavity box, and radiation (e.g., visible light) can be provided to the gain medium to cause emission of microwave radiation.
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What is claimed is: 1. A method of providing microwave amplification, the method comprising: providing a maser system; and providing electromagnetic radiation to the maser system, thereby causing the maser system to emit microwave radiation, wherein the maser system comprises: a gain medium; a resonator disposed around the gain medium; a cavity box disposed around the resonator; and a magnet array disposed around the gain medium, wherein the gain medium comprises diamond having a plurality of nitrogen-vacancy (NV) centers, wherein the electromagnetic radiation is pumped into the cavity box of the maser system at a pump rate that is higher than the decay rate, and wherein a cavity Q factor of the maser system is below a masing threshold of the maser system, such that the maser system operates as a microwave amplifier. 2. The method according to claim 1 , wherein the diamond having a plurality of NV centers is a single-crystal diamond. 3. The method according to claim 1 , wherein the resonator is a sapphire dielectric resonator, and wherein the magnet array has an annulus shape. 4. The method according to claim 1 , wherein the maser system further comprises a support substrate on which the resonator is disposed, wherein the support substrate is disposed within the cavity box. 5. The method according to claim 1 , wherein the system has a cavity Q factor of at least 10,000. 6. The method according to claim 1 , wherein the NV concentration within the diamond gain medium is less than 100 parts per million (ppm). 7. The method according to claim 1 , wherein the cavity box includes an opening to receive radiation, and wherein the maser system further comprises an optical pump disposed outside the cavity box and configured to provide electromagnetic radiation to the gain medium through the opening in the cavity box. 8. The method according to claim 7 , wherein the optical pump is an optical laser, and wherein the electromagnetic radiation is visible light. 9. The method according to claim 1 , wherein the magnet array provides a homogenous magnetic field to the gain medium, and wherein the homogenous magnetic field is at least 1,028 Gauss. 10. The method according to claim 1 , wherein the maser system operates in continuous-wave mode at room temperature, and wherein a power gain of the maser system is at least 6 dB. 11. A method of providing microwave amplification, the method comprising: providing a maser system; and providing electromagnetic radiation to the maser system thereby causing the maser system to emit microwave radiation, wherein the maser system, comprises: a gain medium; a resonator disposed around the gain medium; and a cavity box disposed around the resonator, wherein the gain medium comprises diamond having a plurality of nitrogen-vacancy (NV) centers, wherein the electromagnetic radiation is pumped into the cavity box of the maser system at a pump rate that is higher than the decay rate, and wherein a cavity Q factor of the maser system is below a masing threshold of the maser system, such that the maser system operates as a microwave amplifier. 12. The method according to claim 11 , wherein the diamond having a plurality of NV centers is a single-crystal diamond, wherein the system has a cavity Q factor of at least 10,000, and wherein the NV concentration within the diamond gain medium is less than 100 parts per million (ppm). 13. The method according to claim 11 , wherein the cavity box includes an opening to receive radiation, wherein the maser system further comprises an optical pump disposed outside the cavity box and configured to provide electromagnetic radiation to the gain medium through the opening in the cavity box, wherein the optical pump is an optical laser, and wherein the electromagnetic radiation is visible light. 14. The method according to claim 11 , wherein the maser system operates in continuous-wave mode at room temperature, and wherein a power gain of the maser system is at least 6 dB.
Crystal lasers or glass lasers (H01S3/063 takes precedence) · CPC title
using a relativistic beam of charged particles, e.g. electron cyclotron maser, gyrotron · CPC title
characterised by a crystal matrix · CPC title
solid · CPC title
Devices using stimulated emission of electromagnetic radiation in wave ranges other than those covered by groups H01S1/00, H01S3/00 or H01S5/00, e.g. phonon masers, X-ray lasers or gamma-ray lasers · CPC title
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