System and method for circuit quantum electrodynamics measurement

Patent metadata

Field	Value
Publication number	US-9692423-B2
Application number	US-201414584659-A
Country	US
Kind code	B2
Filing date	Dec 29, 2014
Priority date	Dec 29, 2014
Publication date	Jun 27, 2017
Grant date	Jun 27, 2017

Abstract

A system for quantum computation and a readout method using the same are provided. In some aspects, the system includes at least one qubit circuit coupled to a resonant cavity, wherein each of the at least one qubit circuit is described by multiple quantum states, and a controller configured to provide microwave irradiation to the resonant cavity such that a quantum state information of the at least one qubit circuit is transferred to a resonant cavity occupation. The system also includes a readout circuit, coupled to the resonant cavity, configured to receive signals corresponding to the resonant cavity occupation, and generate an output indicative of the quantum states of the at least one qubit circuit. Optionally, the system further includes at least one single flux quantum (“SFQ”) circuit coupled to the readout circuit and configured to receive the output therefrom.

First claim

What is claimed is:

1. A system for quantum computation comprising:
at least one qubit circuit coupled to a resonant readout cavity, wherein each of the at least one qubit circuit is described by multiple quantum states;
a controller configured to provide microwave irradiation to the resonant readout cavity such that a quantum state information of the at least one qubit circuit is transferred to a resonant cavity occupation; and
a readout circuit, coupled to the resonant readout cavity, configured to receive signals corresponding to the resonant cavity occupation, and generate an output indicative of the quantum states of the at least one qubit circuit.

2. The system of claim 1 , wherein the at least one qubit circuit comprises a transmon qubit.

3. The system of claim 1 , wherein the resonant cavity occupation achieved using the controller comprises a bright cavity pointer state or a dark cavity pointer state.

4. The system of claim 1 , wherein the readout circuit comprises a Josephson photomultiplier (“JPM”) circuit.

5. The system of claim 1 , wherein the output includes a binary signal.

6. The system of claim 1 , wherein the system further comprises at least one single flux quantum (“SFQ”) logic circuit coupled to the readout circuit and configured to receive the output therefrom.

7. The system of claim 6 , wherein the at least one SFQ logic circuit and the readout circuit are coupled using a Josephson transmission line (“JTL”).

8. The system of claim 1 , wherein the readout circuit is coupled to a Josephson transmission line (“JTL”) using a normal metal resistor.

9. The system of claim 1 , wherein the readout circuit is detuned away from a measurement frequency such that an effective interaction between the resonant readout cavity and the readout circuit is dispersive during a drive stage.

10. A readout method for use in quantum computation, the method comprising:
i) applying an excitation to a resonant readout cavity coupled to at least one qubit circuit to achieve a resonant cavity occupation, wherein a frequency of the excitation corresponds to one of a plurality of quantum states of the at least one qubit circuit; and
ii) mapping the resonant cavity occupation to a voltage state of a readout circuit coupled to the resonant readout cavity to generate an output indicative of the quantum states of the at least one qubit circuit.

11. The method of claim 10 , wherein the excitation applied at step i) includes microwave irradiation applied for a duration related to a frequency spacing between dressed states of the resonant readout cavity corresponding to the quantum states of the at least one qubit circuit.

12. The method of claim 10 , wherein at step i) a quantum state information of the at least one qubit circuit is transferred to the resonant cavity occupation.

13. The method of claim 10 , wherein the resonant cavity occupation comprises a bright cavity pointer state or a dark cavity pointer state.

14. The method of claim 10 , wherein the readout circuit includes a Josephson photomultiplier (“JPM”) circuit.

15. The method of claim 14 , the method further comprising biasing a Josephson junction in the JPM circuit below a critical current.

16. The method of claim 10 , wherein at step i) the readout circuit is detuned away from a measurement frequency such that an effective interaction between the resonant readout cavity and the readout circuit is dispersive.

17. The method of claim 10 , wherein mapping the resonant cavity occupation at step ii) comprises applying a bias pulse that tunes the readout circuit into resonance with the resonant readout cavity.

18. The method of claim 10 , wherein the output comprises a binary signal.

19. The method of claim 10 , the method further comprising providing the output to at least one single flux quantum (“SFQ”) logic circuit coupled to the readout circuit.

20. The method of claim 10 , the method further comprising restoring the resonant readout cavity to a near-vacuum state by applying a coherent pulse to depopulate the resonant readout cavity.

Assignees

• Mcdermott Iii Robert Francis
• Plourde Britton Louis Thomas
• Vavilov Maxim George
• Wilhelm-Mauch Frank Karsten
• Govia Luke Colin Gene
• Pritchett Emily Joy
• Wisconsin Alumni Res Found
• Univ Saarland

Inventors

• Mcdermott Iii Robert Francis
• Plourde Britton Louis Thomas
• Vavilov Maxim George
• Wilhelm-Mauch Frank Karsten
• Govia Luke Colin Gene
• Pritchett Emily Joy

Classifications

• G06N99/002

  Physics · mapped topic

• H03K19/1954 Primary

  with injection of the control current · CPC title

• H03K19/195 Primary

  using superconductive devices · CPC title

• H03K19/19

  using ferro-resonant devices · CPC title

• H03K19/1958

  Hybrid configuration, i.e. using electromagnetic coupling and injection of the control current · CPC title