Generation of an entangled photonic state from primitive resources
US-11501198-B1 · Nov 15, 2022 · US
US12198012B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-12198012-B2 |
| Application number | US-202318299821-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 13, 2023 |
| Priority date | Apr 27, 2021 |
| Publication date | Jan 14, 2025 |
| Grant date | Jan 14, 2025 |
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A quantum computing system, method, and computer readable medium involves initializing a state of a resonator-coupled quantum emitter having at least four levels arranged in an N-configuration, the N-configuration having a first ground state, a second ground state, a first excited state and a second excited state. A frequency of a first transition between the first ground state and the first excited state is tuned, a frequency of a second transition between the second ground state and the second excited state is tuned, and a frequency of a third transition between the second ground state and the first excited state is tuned. A plurality of photons are fed at a frequency corresponding to the frequency of the second transition, thereby entangling the plurality of photons to the resonator-coupled quantum emitter. Likewise, a photon at a frequency corresponding to the frequency of at least one of the first transition or the third transition is fed, thereby mapping a state of the resonator-coupled quantum emitter into a photon.
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The invention claimed is: 1. A quantum computing method, comprising: initializing a state of a resonator-coupled quantum emitter having at least four levels arranged in an N-configuration, the N-configuration having a first ground state, a second ground state, a first excited state and a second excited state; tuning a frequency of a first transition between the first ground state and the first excited state; tuning a frequency of a second transition between the second ground state and the second excited state; tuning a frequency of a third transition between the second ground state and the first excited state; feeding a plurality of photons at a frequency corresponding to the frequency of the second transition, thereby entangling the plurality of photons to the resonator-coupled quantum emitter; and feeding a photon at a frequency corresponding to the frequency of at least one of the first transition or the third transition, thereby mapping a state of the resonator-coupled quantum emitter into a photon. 2. The method of claim 1 , wherein the state of a resonator-coupled quantum emitter is an electronic state, a nuclear state, or a combination thereof. 3. The method of claim 1 , wherein the tuning of the frequencies of the first transition, the second transition and the third transition occur before the initializing. 4. The method of claim 1 , wherein the tuning of one or more of the frequencies of the transitions occurs by light-shift using a laser. 5. The method of claim 1 , wherein the tuning of one or more of the frequencies of the transitions occurs by Zeeman shift through application of a magnetic field. 6. The method of claim 1 , wherein feeding a photon at a frequency corresponding to the frequency of at least one of the first transition or the third transition further initializes the resonator-coupled quantum emitter to correspond to at least one of the first ground state or the second ground state. 7. The method of claim 1 , wherein feeding a plurality of photons includes sequentially feeding a plurality of single photons. 8. The method of claim 1 , wherein the initializing of the state of the resonator-coupled quantum emitter includes preparing the resonator-coupled quantum emitter in a superposition state of the first ground state and the second ground state. 9. The method of claim 8 , wherein the superposition state is an equal superposition of the first ground state and the second ground state. 10. The method of claim 1 , wherein the resonator-coupled quantum emitter includes two resonators coupled to a single quantum emitter. 11. The method of claim 1 , wherein the quantum emitter includes a stationary qubit capable of interacting with photons. 12. The method of claim 1 , wherein the quantum emitter includes one of a superconducting qubit or a quantum dot. 13. The method of claim 1 , wherein the quantum emitter includes a neutral atom. 14. The method of claim 1 , wherein the quantum emitter includes an ion. 15. The method of claim 1 , wherein the quantum emitter includes at least one of a rubidium atom or a cesium atom. 16. The method of claim 1 , wherein the quantum emitter includes at least one of Strontium, Erbium, Ytterbium, Calcium, Barium, Beryllium, or Magnesium atom. 17. A quantum computing system, comprising: a resonator-coupled quantum emitter having at least four levels arranged in an N-configuration, the N-configuration having a first ground state, a second ground state, a first excited state and a second excited state; and circuitry configured to: initialize a state of the resonator-coupled quantum emitter; tune a frequency of a first transition between the first ground state and the first excited state; tune a frequency of a second transition between the second ground state and the second excited state; tune a frequency of a third transition between the second ground state and the first excited state; feed a plurality of photons at a frequency corresponding to the frequency of the second transition, thereby entangling the plurality of photons to the resonator-coupled quantum emitter; and feed a photon at a frequency corresponding to a frequency of at least one of the first transition or the third transition, thereby mapping a state of the resonator-coupled quantum emitter into a photon. 18. The system of claim 17 , further comprising at least one of: a laser for light-shifting, thereby tuning at least one of the frequencies of the transitions; or a magnetic field generator for providing a magnetic field, application of the magnetic field for tuning at least one of the frequencies of the transitions. 19. The system of claim 17 , wherein the resonator-coupled quantum emitter includes two resonators coupled to a single quantum emitter. 20. A non-transitory computer-readable medium including instructions that when executed by at least one processor, cause the at least one processor to carry out a quantum computing method, comprising: initializing a state of a resonator-coupled quantum emitter having at least four levels arranged in an N-configuration, the N-configuration having a first ground state, a second ground state, a first excited state and a second excited state; tuning a frequency of a first transition between the first ground state and the first excited state; tuning a frequency of a second transition between the second ground state and the second excited state; tuning a frequency of a third transition between the second ground state and the first excited state; feeding a plurality of photons at a frequency corresponding to the frequency of the second transition, thereby entangling the plurality of photons to the resonator-coupled quantum emitter; and feeding a photon at a frequency corresponding to the frequency of at least one of the first transition or the third transition, thereby mapping a state of the resonator-coupled quantum emitter into a photon.
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