Tunable bus-mediated coupling between remote qubits

Patent metadata

Field	Value
Publication number	US-10353844-B2
Application number	US-201816026573-A
Country	US
Kind code	B2
Filing date	Jul 3, 2018
Priority date	Jan 21, 2016
Publication date	Jul 16, 2019
Grant date	Jul 16, 2019

Abstract

A tunable bus-mediated coupling system is provided that includes a first input port coupled to a first end of a variable inductance coupling element through a first resonator and a second input port coupled to a second end of the variable inductance coupling element through a second resonator. The first input port is configured to be coupled to a first qubit, and the second output port is configured to be coupled to a second qubit. A controller is configured to control the inductance of the variable inductance coupling element between a low inductance state to provide strong coupling between the first qubit and the second qubit and a high inductance state to provide isolation between the first qubit and the second qubit.

First claim

What is claimed is:

1. A tunable bus-mediated coupling system comprising:
a first port coupled to a first end of a variable inductance coupling element through a first resonator, the first port being configured to be coupled to a first qubit;
a second port coupled to a second end of the variable inductance coupling element through a second resonator, the second port being configured to be coupled to a second qubit; and
a controller configured to control inductance of the variable inductance coupling element between a low inductance state to provide strong coupling between the first qubit and the second qubit and a high inductance state to provide isolation between the first qubit and the second qubit.

2. The system of claim 1 , wherein the variable inductance coupling element comprises a series array of N Josephson junctions, each of the N Josephson junctions having a critical current N times larger than a single Josephson junction.

3. The system of claim 1 , wherein the variable inductance coupling element is a Josephson junction.

4. The system of claim 3 , further comprising a first termination inductor coupled between the first resonator and the Josephson junction on a first end and ground on a second end, and a second termination inductor coupled between the second resonator and the Josephson junction on a first end and ground on a second end, wherein the first termination inductor, the Josephson junction and the second termination inductor form an RF-SQUID.

5. The system of claim 4 , further comprising a bias inductor inductively coupled to one of the first termination inductor and the second termination inductor, wherein an amount of current through the bias inductor controls the coupling strength between the first and the second qubit.

6. The system of claim 4 , further comprising a first coupling capacitor coupled between the first port and the first resonator, and a second coupling capacitor coupled between the second port and the second resonator.

7. The system of claim 5 , wherein the controller controls an amount of current through the bias inductor inductively coupled to one of the first and the second termination inductors.

8. The system of claim 7 , wherein the controller provides a current through the bias inductor between no current that induces no net flux in the RF-SQUID allowing for coupling between the first and second qubit and a current that induces a net flux in the RF-SQUID of 0.1 Φ 0 to 0.45 Φ 0 , where Φ 0 is equal to a flux quantum, providing isolation between the first and second qubit.

9. A superconducting system comprising the tunable bus-mediated coupling system of claim 1 , the superconducting system comprising a first qubit system comprising the first qubit, and a second qubit system remote from the first qubit system and comprising the second qubit, wherein the tunable bus-mediated coupling system is arranged to couple and decouple the first qubit and second qubit.

10. A superconducting system comprising:
a first qubit system comprising a first qubit;
a second qubit system remote from the first qubit system and comprising a second qubit;
a tunable bus-mediated coupler disposed between the first qubit and the second qubit, the tunable bus-mediated coupler having a first state for strongly coupling the first qubit to the second qubit and a second state for isolating the first qubit to the second qubit, the tunable bus-mediated coupler comprising a variable inductance coupling element disposed between a first resonator coupled to the first qubit and a second resonator coupled to the second qubit; and
a controller configured to control the inductance of the variable inductance coupling element between a low inductance state to provide strong coupling between the first qubit and the second qubit and a high inductance state to provide isolation between the first qubit and the second qubit.

11. The system of claim 10 , wherein the variable inductance coupling element is a Josephson junction.

12. The system of claim 11 , further comprising a first termination inductor coupled between the first resonator and the Josephson junction on a first end and ground on a second end, and a second termination inductor coupled between the second resonator and the Josephson junction on a first end and ground on a second end, wherein the first termination inductor, the Josephson junction and the second termination inductor form an RF-SQUID.

13. The system of claim 12 , further comprising a bias inductor inductively coupled to one of the first termination inductor and the second termination inductor, wherein an amount of current through the bias inductor controls the coupling strength between the first and the second qubit.

14. The system of claim 13 , further comprising a first coupling capacitor coupled between the first qubit and the first resonator, and a second coupling capacitor coupled between the second resonator and the second qubit.

15. The system of claim 13 , wherein the controller provides a current through the bias inductor between no current that induces no net flux in the RF-SQUID allowing for coupling between the first and second qubit and a current that induces a net flux in the RF-SQUID of 0.1 Φ 0 to 0.45 Φ 0 , where Φ 0 is equal to a flux quantum, providing isolation between the first and second qubit.

16. A superconducting system comprising:
a first qubit system comprising a first qubit;
a second qubit system remote from the first qubit system and comprising a second qubit; and
a tunable bus-mediated coupler disposed between the first qubit and the second qubit, the tunable bus-mediated coupler comprising:
a first port coupled to a first end of a Josephson junction through a first resonator, the first port being coupled to the first qubit;
a second port coupled to a second end of the Josephson junction through a second resonator, the second port being coupled to the second qubit;
a first termination inductor coupled between the first resonator and the Josephson junction on a first end and ground on a second end, and
a second termination inductor coupled between the second resonator and the Josephson junction on a first end and ground on a second end, wherein the first termination inductor, the Josephson junction and the second termination inductor form an RF-SQUID;

a bias inductor inductively coupled to one of the first termination inductor and the second termination inductor, wherein an amount of current through the bias inductor controls the coupling strength between the first and the second qubit; and
a controller that controls an amount of current through the bias inductor inductively coupled to one of the first and the second termination inductors to control the inductance of the Josephson junction between a low inductance state to provide strong coupling between the first qubit and the second qubit and a high inductance state to provide isolation between the first qubit and the second qubit.

17. The system of claim 16 , further comprising a first coupling capacitor coupled between the first qubit and the first resonator, and a second coupling capacitor coupled between the second resonator and the second qubit.

18. The system of claim 16 , wherein the controller provides a current through the bias inductor between no current that induces no net flux in the RF-SQUID allowing for coupling between the first and second qubit and a current that induces a net flux in the RF-SQUID of 0.1 Φ 0 to 0.45 Φ 0 , where Φ 0 is equal to a flux quantum, providing isolation between the first and second qubit.

Assignees

• Naaman Ofer
• Keane Zachary Kyle
• Stoutimore Micah John Atman
• Ferguson David George
• Northrop Grumman Systems Corp

Inventors

• Naaman Ofer
• Keane Zachary Kyle
• Stoutimore Micah John Atman
• Ferguson David George

Classifications

• G06F13/4027 Primary

  using bus bridges (G06F13/4022 takes precedence) · CPC title

• G06F13/4068

  Electrical coupling · CPC title

• H01L39/025

  Electricity · mapped topic

• G06N10/00

  Quantum computing, i.e. information processing based on quantum-mechanical phenomena · CPC title

• H01L39/223

  Electricity · mapped topic