Coherent quantum information transfer between conventional qubits

Patent metadata

Field	Value
Publication number	US-2015242758-A1
Application number	US-201314064828-A
Country	US
Kind code	A1
Filing date	Oct 28, 2013
Priority date	Nov 10, 2010
Publication date	Aug 27, 2015
Grant date	—

Abstract

Computing bus devices that enable quantum information to be coherently transferred between conventional qubit pairs are disclosed. A concrete realization of such a quantum bus acting between conventional semiconductor double quantum dot qubits is described. The disclosed device measures the joint (fermion) parity of the two qubits by using the Aharonov-Casher effect in conjunction with an ancillary superconducting flux qubit that facilitates the measurement. Such a parity measurement, together with the ability to apply Hadamard gates to the two qubits, allows for the production of states in which the qubits are maximally entangled, and for teleporting quantum states between the quantum systems.

First claim

1 .- 17 . (canceled)

18 . The method of claim 23 , where performing the joint parity measurement on the at least portions of the first and the second non-topological qubits, comprises:
teleporting a quantum state between a third non-topological qubit and at least one of the first and the second non-topological qubits.

19 .- 22 . (canceled)

23 . A method for performing quantum operations on non-topological qubits, the method comprising:
coupling a first non-topological qubit and a second non-topological qubit using a flux qubit using an Aharonov Casher effect, wherein the first non-topological qubit and the second non-topological qubit are first and second charge double-dot qubits, respectively, wherein first portions of the first and the second charge double-dot qubits are proximal to the flux qubit, wherein the flux qubit has first, second and third Josephson junctions, wherein the first portion of the first charge double-dot qubit interposes the first and the second Josephson junctions, the first portion of the second charge double-dot qubit interposes the second and the third Josephson junctions, and the first non-topological qubit and the second non-topological qubit are coupled based on a phase difference associated with the first and third Josephson junctions produced by the Aharonov-Casher effect; and performing a joint parity measurement on at least the portion of the first non-topological qubit and at least the portion of the second non-topological qubit.

24 . The method of claim 23 , wherein performing the joint parity measurement on the first and the second non-topological qubits comprises: performing the joint parity measurement on first dots of the first and the second charge double-dot qubits.

25 . The method of claim 23 , further comprising:
performing a joint parity measurement on at least a portion of a third non-topological qubit and another portion of the first non-topological qubit.

26 . The method of claim 25 , wherein performing the joint parity measurement on the third non-topological qubit and the other portion of the first non-topological qubit comprises:
entangling the third non-topological qubit with the second non-topological qubit.

27 . The method of claim 26 , wherein entangling the third non-topological qubit with the second non-topological qubit comprises:
teleporting a quantum state between the second non-topological qubit and the third non-topological qubit.

28 . The method of claim 12 claim 23 , wherein the first and the second non-topological qubits are coupled via the joint parity measurement, the method further comprising:
decoupling the first and the second non-topological qubits.

29 . The method of claim 28 , wherein decoupling the first and the second non-topological qubits further comprises:
tuning a flux away from a degeneracy point.

30 - 36 . (canceled)

37 . A method for performing quantum operations on non-topological qubits, the method comprising:
coupling a first non-topological qubit and a second non-topological qubit using a flux qubit using an Aharonov Casher effect, wherein portions of the first and the second non-topological qubits are proximal to the flux qubit, wherein the flux qubit has first, second and third Josephson junctions, wherein the portion of the first non-topological qubit interposes the first and the second Josephson junctions, the portion of the second non-topological qubit interposes the second and the third Josephson junctions, and the first non-topological qubit and the second non-topological qubit are coupled based on a phase difference associated with the first and third Josephson junctions produced by the Aharonov-Casher effect; and performing a joint parity measurement on at least the portion of the first non-topological qubit and at least the portion of the second non-topological qubit.

38 . The method of claim 37 , wherein at least one of the first and the second non-topological qubits is a charge double-dot qubit.

39 . The method of claim 37 , wherein performing the joint parity measurement on the at least portions of the first and the second non-topological qubits, comprises:
teleporting a quantum state between a third non-topological qubit and at least one of the first and the second non-topological qubits.

Assignees

• Microsoft Corp

Inventors

• Bonderson Parsa
• Lutchyn Roman M

Classifications

• H10N60/12 Primary

  Josephson-effect devices · CPC title

• H01L39/025

  Electricity · mapped topic

• G06N99/002 Primary

  Physics · mapped topic

• H01L39/223

  Electricity · mapped topic

• B82Y10/00

  Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic · CPC title