Quantum nondemolition microwave photon counter based on the cross-kerr nonlinearity of a josephson junction embedded in a superconducting circuit
View Patent ↗A technique relates to a microwave device. A pump resonator, at a first pump resonator end, is connected to both a dispersive nonlinear element and a first stub. The pump resonator, at a second pump resonator end, is capacitively coupled to a pump port, where the first stub is terminated in an open circuit. A quantum signal resonator, at a first quantum signal resonator end, is connected to both the dispersive nonlinear element and a second stub. The quantum signal resonator, at a second signal resonator end, is capacitively coupled to a signal port, where the second stub is connected to ground.
1. A system comprising:
a quantum device configured to output a quantum signal;
a microwave device coupled to the quantum device, the microwave device comprising:
a first resonator coupled to both a dispersive nonlinear element and a first stub; and
a second resonator coupled to both the dispersive nonlinear element and a second stub, wherein one of the first and second stubs is connected to an open circuit.
2. The system of claim 1 , further comprising a measurement device coupled to the first resonator or the second resonator.
3. The system of claim 2 , wherein the measurement device is configured to measure a reflected pump signal having interacted with the microwave device.
4. The system of claim 3 , wherein the measurement device is configured to determine an absence or presence of photons in the quantum signal having been input according to a phase shift in the reflected pump signal.
5. The system of claim 4 , wherein a number of photons in the quantum signal is determined by a magnitude of the phase shift in the reflected pump signal.
6. The system of claim 1 , wherein the quantum device is coupled to the first resonator or the second resonator.
7. The system of claim 1 , wherein the quantum device comprises a qubit and the quantum signal is associated with the qubit.
8. The system of claim 1 , wherein the first stub is coupled to the dispersive nonlinear element.
9. The system of claim 1 , wherein the second stub is coupled to the dispersive nonlinear element.
10. The system of claim 1 , wherein one of the first and second stubs is connected to ground.
11. A microwave device comprising:
a first resonator coupled to both a dispersive nonlinear element and a first stub; and
a second resonator coupled to both the dispersive nonlinear element and a second stub, wherein the first resonator comprises a pump resonance mode, the pump resonance mode having a pump resonance frequency and a pump wavelength, and a length of the first resonator corresponding to a quarter wavelength of the pump wavelength.
12. The microwave device of claim 11 , wherein the first resonator is operable to couple to a measurement device.
13. The microwave device of claim 11 , wherein the first resonator is operative to couple to a pump signal source.
14. The microwave device of claim 11 , wherein the second resonator is operable to couple to a quantum device.
15. The microwave device of claim 11 , wherein the second resonator is operable to couple to a 50 ohm termination point.
16. The microwave device of claim 11 , wherein the dispersive nonlinear element is at least one Josephson junction.
17. The microwave device of claim 11 , wherein the dispersive nonlinear element is an array of Josephson junctions.
18. The microwave device of claim 11 , wherein the second resonator comprises a signal resonance mode, the signal resonance mode having a signal resonance frequency and a signal wavelength, a length of the second resonator corresponding to a quarter wavelength of the signal wavelength.
19. The microwave device of claim 11 , wherein the first resonator, the second resonator, the first and second stubs, and the dispersive nonlinear element are configured to neither destroy nor absorb any photons input in a quantum signal.