Light-emitting device and light source apparatus
US-10651027-B2 · May 12, 2020 · US
US10824048B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10824048-B2 |
| Application number | US-201916373605-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 2, 2019 |
| Priority date | Apr 2, 2019 |
| Publication date | Nov 3, 2020 |
| Grant date | Nov 3, 2020 |
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A electronic method, includes receiving, by a graphene structure, a microwave signal. The microwave signal has a driving voltage level. The electronic method includes generating, by the graphene structure, optical photons based on the microvolts. The electronic method includes outputting, by the graphene structure, the optical photons.
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What is claimed is: 1. An electronic method for converting from a microwave to an optical domain, comprising: receiving, by a graphene structure, microvolts, wherein the microvolts are sent to the graphene structure via a microwave signal, and the microwave signal is received by the graphene structure at a quantum level, and wherein the graphene structure is receiving the microvolts at a particular cryogenic temperature, generating, by the graphene structure, optical photons based on receiving the microvolts; and outputting, by the graphene structure, the optical photons at the quantum level, wherein: the graphene structure is a quantum modulator which generates the optical photons based on the received microvolts, and the generating the optical photons is based on a microwave frequency of different electron densities. 2. The electronic method of claim 1 , wherein the graphene structure has multiple graphene layers, wherein: the multiple graphene layers have a distance, d, from each other, the multiple graphene layers are connected with each other in an interdigital configuration and operate electronically as a capacitor and, at the same time, operate optically as a periodic medium, and wherein each of the graphene layers has an area of 1 mm 2 . 3. The electronic method of claim 1 , where the graphene structure has multiple graphene layers, wherein each of the multiple graphene layers has a length L, wherein the length is less than 2.0 millimeters. 4. The electronic method of claim 1 , wherein the driving voltage is less than 10 microvolts and the particular cryogenic temperature is in milli-Kelvins. 5. The electronic method of claim 1 , wherein the graphene structure is pumped by an optical pump, wherein: the optical pump has an intensity level that is below a damage threshold level of the graphene structure, and the optical pump has an amplitude, |A 1 | of A 1 = π v g 2 L g , wherein, v g is a group velocity, L is a length of the graphene structure, and |g| is a conversion rate associated with converting microvolts to optical photons at the quantum state. 6. The electronic method of claim 1 , further comprising: generating, by the graphene structure, a lower sideband, wherein the lower sideband is generated based on the microwave signal modulating the graphene structure's effective permittivity; suppressing, by the graphene structure, the lower sideband generated when the graphene structure is pumped by an optical pump, wherein the lower sideband is suppressed to a destruction resonance value associated with the graphene structure and wherein no reflected waves are generated at the lower sideband; generating, by the graphene structure, an upper sideband at the same time that the lower sideband is generated, wherein a quantum state of the upper sideband only depends on a microwave signal, wherein the microvolts is sent to the graphene structure via the microwave signal. 7. The electronic method of claim 1 , wherein the graphene structure has multiple graphene layers that are connected to each other in an interdigital configuration. 8. The electronic method of claim 1 , wherein a conversion rate, associated with generating the optical photons from the microvolts is based on a length of the graphene structure and the optical pump amplitude.
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