Driving the common-mode of a josephson parametric converter using a three-port power divider
US-9548742-B1 · Jan 17, 2017 · US
US9680452B1 · US · B1
| Field | Value |
|---|---|
| Publication number | US-9680452-B1 |
| Application number | US-201615295251-A |
| Country | US |
| Kind code | B1 |
| Filing date | Oct 17, 2016 |
| Priority date | Oct 17, 2016 |
| Publication date | Jun 13, 2017 |
| Grant date | Jun 13, 2017 |
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A technique relates to a circuit for a sum frequency generator. A first resonator is connected to a Josephson ring modulator (JRM), and the first resonator is configured to receive a first photon at a first frequency. A second resonator is connected to the JRM, and the second resonator is configured to have a first harmonic and no second harmonic. The second resonator is configured to receive a second photon at a second frequency, and the first resonator is configured to output an up-converted photon. The up-converted photon has an up-converted frequency that is a sum of the first frequency and the second frequency.
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What is claimed is: 1. A circuit for a sum frequency generator, the circuit comprising: a first resonator connected to a Josephson ring modulator (JRM), wherein the first resonator is configured to receive a first photon at a first frequency; and a second resonator connected to the JRM, the second resonator configured to have a first harmonic and no second harmonic, wherein the second resonator is configured to receive a second photon at a second frequency, wherein the first resonator is configured to output an up-converted photon, the up-converted photon having an up-converted frequency that is a sum of the first frequency and the second frequency. 2. The circuit of claim 1 , wherein a fundamental resonance frequency is about a same for the first resonator and the second resonator. 3. The circuit of claim 2 , wherein the first frequency of the first photon and the second frequency of the second photon are about a same. 4. The circuit of claim 1 , wherein a fundamental resonance frequency of the second resonator is higher than the first resonator. 5. The circuit of claim 4 , wherein the second frequency of the second photon is higher than the first frequency of the first photon. 6. The circuit of claim 1 , wherein the first resonator has a second harmonic configured to output the up-converted photon at the up-converted frequency; wherein the up-converted photon is a sum of energy from the first photon and the second photon. 7. The circuit of claim 1 , wherein the first resonator is a half-wavelength transmission line resonator. 8. The circuit of claim 7 , wherein the second resonator is a lumped-element resonator. 9. The circuit of claim 1 , wherein the first resonator is formed of microstrips. 10. The circuit of claim 1 , wherein the second resonator is formed of capacitors, each having a top plate connected to the JRM and a bottom plate connected together, separated by a dielectric substrate or medium. 11. A method of forming a circuit for a sum frequency generator, the method comprising: providing a first resonator connected to a Josephson ring modulator (JRM), wherein the first resonator is configured to receive a first photon at a first frequency; and providing a second resonator connected to the JRM, the second resonator configured to have a first harmonic and no second harmonic, wherein the second resonator is configured to receive a second photon at a second frequency, wherein the first resonator is configured to output an up-converted photon, the up-converted photon having an up-converted frequency that is a sum of the first frequency and the second frequency. 12. The method of claim 11 , wherein a fundamental resonance frequency is about a same for the first resonator and the second resonator. 13. The method of claim 12 , wherein the first frequency of the first photon and the second frequency of the second photon are about a same. 14. The method of claim 11 , wherein a fundamental resonance frequency of the second resonator is higher than the first resonator. 15. The method of claim 14 , wherein the second frequency of the second photon is higher than the first frequency of the first photon. 16. The method of claim 11 , wherein the first resonator has a second harmonic configured to output the up-converted photon at the up-converted frequency; wherein the up-converted photon is a sum of energy from the first photon and the second photon. 17. The method of claim 11 , wherein the first resonator is a half-wavelength transmission line resonator. 18. The method of claim 17 , wherein the second resonator is a lumped-element resonator. 19. The method of claim 11 , wherein the first resonator is formed of microstrips. 20. The method of claim 11 , wherein the second resonator is formed of capacitors, each having a top plate connected to the JRM and a bottom plate connected together, separated by a dielectric substrate or medium. 21. A method for remote entanglement of a first qubit and a second qubit, the method comprising: providing a sum frequency generator circuit separately connected to a first quantum system and a second quantum system, the first quantum system including the first qubit and the second quantum system including the second qubit; and remotely entangling the first qubit and the second qubit which includes: causing the first quantum system to transmit a first output readout signal at a first frequency to the sum frequency generator and causing the second quantum system to transmit a second output readout signal at a second frequency to the sum frequency generator circuit, and outputting, by the sum frequency generator, an up-converted output readout signal having an up-converted frequency that is a sum of the first frequency and the second frequency, thereby remotely entangling the first qubit and the second qubit. 22. The method of claim 21 , wherein the first output readout signal includes state information of the first qubit and the second output readout signal includes state information of the second qubit. 23. The method of claim 22 , wherein the up-converted output readout signal is a superposition of the state information of the first and the second qubits. 24. A method for configuring a microwave repeater, the method comprising: providing a first sum frequency generator through a last sum frequency generator; and providing a first spontaneous parametric down-conversion device through a last spontaneous parametric down-conversion device; wherein each of the first through last sum frequency generators is connected to two of the first through last spontaneous parametric down-conversion devices, such that each one of the first through last sum frequency generators is shared by two of the first through last spontaneous parametric down-conversion devices; and wherein a total of the first through last sum frequency generators is one less than a total of the first through last spontaneous parametric down-conversion devices. 25. The method of claim 24 , wherein: a first photon generated by the first spontaneous parametric down-conversion device is received by none of the first through last sum frequency generators; a last photon generated by the last spontaneous parametric down-conversion device is received by none of the first through last sum frequency generators; the first through last sum frequency generators are configured to cause remote entanglement of the first and second photons; and the first through the third spontaneous parametric down-conversion devices are nondegenerate, three-wave mixing amplifiers.
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