SYSTEMS, DEVICES, AND METHODS FOR CONTROLLABLY COUPLING QUBITS

• US 20090078932A1
• Filed: 09/25/2008
• Published: 03/26/2009
• Est. Priority Date: 09/25/2007
• Status: Active Grant

• Current Assignee: D-Wave Systems Inc. (D-Wave Quantum, Inc.)
• Original Assignee: D-Wave Systems Inc. (D-Wave Quantum, Inc.)
• Inventors: Amin, Mohammad H.
• Granted Patent: US 7,880,529 B2
• Time in Patent Office: Days
• US Class Current: 257/31
• CPC Class Codes: B82Y 10/00 Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
• CPC Class Codes: G06N 10/00 Quantum computing, i.e. information processing based on quantum-mechanical phenomena

Abstract

A coupling system may include first and second magnetic flux inductors communicatively coupled to a Josephson junction of an rf SQUID. The coupling system may allow transverse coupling between qubits. A superconducting processor may include at least one of the coupling systems and two or more qubits. A method may include providing first, second and third coupling structure to control the coupling system.

Claims

1. A coupling system comprising:

an rf SQUID having a loop of superconducting material interrupted by a compound Josephson junction;

a first magnetic flux inductor inductively coupled to the compound Josephson junction and capable of controlling a β

_L parameter of the coupling system;

a second magnetic flux inductor inductively coupled to the loop of superconducting material;

a first coupling structure coupling the rf SQUID to a first qubit; and

a second coupling structure coupling the rf SQUID to a second qubit; and

wherein the coupling system is operated such that the β

_L parameter is greater than 1.

2. The coupling system of claim 1 wherein at least one of the first qubit and the second qubit is a superconducting flux qubit.

3. The coupling system of claim 1 wherein the first magnetic flux inductor and the second magnetic flux inductor control a coupling state of the rf SQUID.

4. The coupling system of claim 3 wherein the coupling state of the rf SQUID is at least one of an anti-ferromagnetic coupling state, a ferromagnetic coupling state, a transverse coupling state and a zero coupling state.

5. The coupling system of claim 4 wherein the transverse coupling state is in a flux basis.

6. The coupling system of claim 1 wherein the β

_L parameter is controlled by adjusting an amount of flux produced by the first magnetic flux inductor.

7. A method of controllably coupling a first qubit to a second qubit using an rf SQUID having a loop of superconducting material interrupted by a compound Josephson junction, the method comprising:

coupling the first qubit to the rf SQUID;

coupling the second qubit to the rf SQUID;

coupling a first magnetic flux inductor to the compound Josephson junction;

coupling a second magnetic flux inductor to the loop or superconducting material;

adjusting a first amount of flux, produced by the first magnetic flux inductor, threading the compound Josephson junction; and

adjusting a second amount of flux, produced by the second magnetic flux inductor, that threads the loop of superconducting material such that the first qubit is transversely coupled to the second qubit.

8. The method of claim 7 wherein at least one of the first qubit and the second qubit is a superconducting flux qubit.

9. The method of claim 7 wherein coupling the first qubit to the rf SQUID comprises:

threading magnetic flux produced by current flowing in the first qubit into the loop of superconducting material; and

threading magnetic flux produced by current flowing in the loop of superconducting material into the first qubit.

10. The method of claim 7 wherein coupling the second qubit to the rf SQUID comprises:

threading magnetic flux produced by current flowing in the second qubit into the loop of superconducting material; and

threading magnetic flux produced by current flowing in the loop of superconducting material into the second qubit.

11. The method of claim 7 wherein coupling a first magnetic flux inductor to the compound Josephson junction comprises:

threading magnetic flux produced by current flowing through the first magnetic flux inductor into the compound Josephson junction; and

wherein coupling a second magnetic flux inductor to the loop of superconducting material comprises;

threading magnetic flux produced by current flowing through the second magnetic flux inductor into the loop of superconducting material.

12. The method of claim 7 wherein adjusting the amount of flux, produced by the first magnetic flux inductor, threading the compound Josephson junction comprises at least one of passing more current through the first magnetic flux inductor or passing less current through the first magnetic flux inductor;

and

wherein adjusting the amount of flux, produced by the second magnetic flux inductor, threading the loop of superconducting material comprises at least one of passing more current through the second magnetic flux inductor or passing less current through the second magnetic flux inductor.

13. The method of claim 7 wherein adjusting the amount of flux, produced by the first magnetic flux inductor, threading the compound Josephson junction and adjusting the amount of flux, produced by the second magnetic flux inductor, threading the loop of superconducting material result in coupling the first qubit and the second qubit with at least one of an anti-ferromagnetic coupling, a ferromagnetic coupling, a transverse coupling and a zero coupling.

14. The method of claim 7 wherein the first qubit is transversely coupled to the second qubit in a flux basis.

15. A coupling system comprising:

an rf SQUID having a loop of superconducting material interrupted by a compound Josephson junction and a β

_L parameter;

a first magnetic flux inductor configured to selectively provide a first magnetic flux inductor mutual inductance coupling the first magnetic flux inductor to the compound Josephson junction, wherein the first magnetic flux inductor adjusts the β

_L parameter to be greater than one; and

a second magnetic flux inductor configured to selectively provide a second magnetic flux inductor mutual inductance coupling the second magnetic flux inductor to the loop or superconducting material, wherein the loop of superconducting material is positioned with respect to a first qubit to provide a first mutual inductance coupling the rf SQUID to the first qubit, and wherein the loop of superconducting material is positioned with respect to a second qubit to provide a second mutual inductance coupling rf SQUID to the second qubit.

16. A superconducting processor comprising:

a first qubit;

a second qubit;

an rf SQUID having a loop of superconducting material interrupted by a compound Josephson junction and a β

_L parameter;

a first magnetic flux means for selectively providing inductance coupling the first magnetic flux means to the compound Josephson junction, wherein the first magnetic flux means adjusts the β

_L parameter to be greater than one; and

a second magnetic flux means for selectively providing inductance coupling the second magnetic flux means to the loop of superconducting material, wherein the loop of superconducting material is configured to provide a first mutual inductance coupling the rf SQUID to the first qubit and to provide a second mutual inductance coupling the rf SQUID to the second qubit.

17. The superconducting processor of claim 16 wherein at least one of the first qubit and the second qubit is a superconducting flux qubit.

18. The superconducting processor of claim 16 wherein the first magnetic flux means includes a first magnetic flux inductor configured to selectively provide a third mutual inductance coupling the first magnetic flux inductor to the compound Josephson junction.

19. The superconducting processor of claim 16 wherein the second magnetic flux means includes a second magnetic flux inductor configured to selectively provide a fourth mutual inductance coupling the second magnetic flux inductor to the loop of superconducting material.

20. A method of controllably coupling a first qubit to a second qubit using an rf SQUID having a loop of superconducting material interrupted by a compound Josephson junction and a β

_L parameter, the method comprising;

coupling the first qubit to the rf SQUID;

coupling the second qubit to the rf SQUID;

coupling a first magnetic flux inductor to the compound Josephson junction;

coupling a second magnetic flux inductor to the loop or superconducting material;

adjusting a first amount of flux, produced by the second magnetic flux inductor, threading the compound Josephson junction, wherein the first amount of flux adjusts the β

_L parameter to be greater than one; and

adjusting a second amount of flux, produced by the second magnetic flux inductor, threading the loop of superconducting material.

21. The method of claim 20 wherein at least one of the first qubit and the second qubit is a superconducting flux qubit.

22. The method of claim 20 wherein coupling the first qubit to the rf SQUID comprises:

threading magnetic flux produced by current flowing in the first qubit into the loop of superconducting material; and

threading magnetic flux produced by current flowing in the loop of superconducting material into the first qubit.

23. The method of claim 20 wherein coupling the second qubit to the rf SQUID comprises:

threading magnetic flux produced by current flowing in the second qubit into the loop of superconducting material; and

threading magnetic flux produced by current flowing in the loop of superconducting material into the second qubit.

24. The method of claim 20 wherein coupling a first magnetic flux inductor to the compound Josephson junction comprises:

threading magnetic flux produced by current flowing through the first magnetic flux inductor into the compound Josephson junction; and

wherein coupling a second magnetic flux inductor to the loop of superconducting material comprises;

threading magnetic flux produced by current flowing through the second magnetic flux inductor into the loop of superconducting material.

25. The method of claim 20 wherein adjusting the amount of flux, produced by the first magnetic flux inductor, threading the compound Josephson junction comprises at least one of passing more current through the first magnetic flux inductor or passing less current through the first magnetic flux inductor;

and

wherein adjusting the amount of flux, produced by the second magnetic flux inductor, threading the loop of superconducting material comprises at least one of passing more current through the second magnetic flux inductor or passing less current through the second magnetic flux inductor.

26. The method of claim 20 wherein adjusting the amount of flux, produced by the first magnetic flux inductor, threading the compound Josephson junction and adjusting the amount of flux, produced by the second magnetic flux inductor, threading the loop of superconducting material result in coupling the first qubit and the second qubit with at least one of an anti-ferromagnetic coupling, a ferromagnetic coupling, a transverse coupling and a zero coupling.

27. The method of claim 20 wherein the transverse coupling is in a flux basis.