Multimode josephson parametric converter: coupling josephson ring modulator to metamaterial
AssigneeInternational Business Machines Corporation
InventorBaleegh Abdo
Life of this patent
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Abstract
A technique relates to operating a multimode Josephson parametric converter as a multimode quantum limited amplifier. The multimode Josephson parametric converter receives multiple quantum signals in parallel at different resonance frequencies. The multimode Josephson parametric converter amplifies simultaneously the multiple quantum signals, according to pump signals applied to the multimode Josephson parametric converter. The multiple quantum signals having been amplified at the different resonance frequencies are reflected, according to the pump signals.
Claims22
A method of operating a multimode Josephson parametric converter as a multimode quantum limited amplifier, the method comprising:
- receiving, by the multimode Josephson parametric converter, multiple quantum signals in parallel at different resonance frequencies;
- amplifying simultaneously, by the multimode Josephson parametric converter, the multiple quantum signals, according to pump signals applied to the multimode Josephson parametric converter;
- and
- reflecting the multiple quantum signals having been amplified at the different resonance frequencies, according to the pump signals.
A method of operating a multimode Josephson parametric converter to generate multiple pairs of entangled photons, the method comprising:
- receiving, by a first multimode resonator in the multimode Josephson parametric converter, a first group of signals at different resonance frequencies of the resonance modes of the first multimode resonator, wherein the first multimode resonator is a first left-handed transmission line;
- receiving, by a second multimode resonator in the multimode Josephson parametric converter, a second group of signals at different resonance frequencies of the resonance modes of the second multimode resonator, wherein the second multimode resonator is a second left-handed transmission line;
- receiving pump signals, by the second multimode resonator, wherein the pump signals are a first frequency sum through a last frequency sum;
- and
- generating simultaneously pairs of entangled photons, the pairs of entangled photons including a first pair through a last pair.
A method of remote entanglement of multiple qubits by measurement, the method comprising:
- receiving, by a first multimode resonator in the multimode Josephson parametric converter, a first group of readout signals resonant with resonance modes of the first multimode resonator, wherein the first multimode resonator is a first left-handed transmission line;
- receiving, by a second multimode resonator in the multimode Josephson parametric converter, a second group of readout signals resonant with resonance modes of the second multimode resonator, wherein the second multimode resonator is a second left-handed transmission line;
- receiving pump signals, by the second multimode resonator, wherein the pump signals are a first frequency sum through a last frequency sum;
- and
- generating, by the Josephson parametric converter, a first qubit pair based on the first frequency sum through a last qubit pair based on the last frequency sum.
A method of generating a bell state using photons as quantum bits, the method comprising:
- providing a first multimode resonator and a second multimode resonator both connected to a dispersive nonlinear medium, wherein the first multimode resonator is a first left-handed transmission line and the second multimode resonator is a second left-handed transmission line, wherein resonance modes are identical in the first and second multimode resonators;
- receiving, by the second multimode resonator, a pump signal at a frequency sum, the frequency sum is a summation of a resonance frequency of the resonance modes plus a another resonance frequency of the resonance modes;
- and
- generating a first photon and a second photon in an equal superposition of spatial states, the equal superposition of the spatial states for the first and second photons are related to being in the first multimode resonator and the second multimode resonator.
The method of 19, wherein the equal superposition of the spatial states for the first photon is configured such that the first photon has an equal probability of being in the first multimode resonator or the second multimode resonator.
The method of 20, wherein the equal superposition of the spatial states for the second photon is configured such that the second photon has an equal probability of being in the first multimode resonator or the second multimode resonator.
The method of 21, wherein the first photon and the second photon are not both in a same one of the first and second multimode resonators.
Dependencies are inferred from the claim text.