Techniques of oscillator control for quantum information processing and related systems and methods

US10540602B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10540602-B2
Application numberUS-201615552998-A
CountryUS
Kind codeB2
Filing dateFeb 26, 2016
Priority dateFeb 27, 2015
Publication dateJan 21, 2020
Grant dateJan 21, 2020

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  1. Title

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  2. Abstract

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  5. First independent claim

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Abstract

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According to some aspects, a method is provided of operating a circuit quantum electrodynamics system that includes a physical qubit dispersively coupled to a quantum mechanical oscillator, the method comprising applying a first electromagnetic pulse to the physical qubit based on a number state of the quantum mechanical oscillator, wherein the first electromagnetic pulse causes a change in state of the quantum mechanical oscillator, and applying, subsequent to application of the first electromagnetic pulse, a second electromagnetic pulse to the quantum mechanical oscillator that coherently adds or removes energy from the quantum mechanical oscillator.

First claim

Opening claim text (preview).

What is claimed is: 1. A method of operating a circuit quantum electrodynamics system that includes a physical qubit dispersively coupled to a quantum mechanical oscillator, the method comprising: applying a first electromagnetic pulse to the physical qubit based on a number state of the quantum mechanical oscillator, wherein the first electromagnetic pulse causes a change in state of the quantum mechanical oscillator; and applying, subsequent to application of the first electromagnetic pulse, a second electromagnetic pulse to the quantum mechanical oscillator that coherently adds or removes energy from the quantum mechanical oscillator. 2. The method of claim 1 , further comprising: driving the physical qubit to a ground state prior to application of the first electromagnetic pulse; and driving the physical qubit to the ground state after application of the first electromagnetic pulse. 3. The method of claim 1 , further comprising measuring a parity of the quantum mechanical oscillator by applying a third electromagnetic pulse to the physical qubit based on the number state of the quantum mechanical oscillator. 4. The method of claim 1 , further comprising measuring the number state of the quantum mechanical oscillator by applying a fourth electromagnetic pulse to the physical qubit. 5. The method of claim 1 , wherein a frequency of the first electromagnetic pulse is based on the number state of the quantum mechanical oscillator. 6. The method of claim 1 , wherein an amplitude of the first electromagnetic pulse is less than a magnitude of a dispersive coupling between the physical qubit and the quantum mechanical oscillator. 7. The method of claim 1 , wherein the change in state of the quantum mechanical oscillator caused by the first electromagnetic pulse is a quantum phase change of one or more Fock state components of the quantum mechanical oscillator. 8. The method of claim 1 , wherein a qubit frequency shift per photon in the quantum mechanical oscillator is larger than a qubit transition line width. 9. The method of claim 1 , wherein the first electromagnetic pulse includes a first frequency component and wherein the quantum mechanical oscillator is resonant at a second frequency, different from the first frequency. 10. The method of claim 1 , wherein a frequency of the second electromagnetic pulse is a resonant frequency of the quantum mechanical oscillator. 11. The method of claim 1 , wherein the second electromagnetic pulse is based at least in part on the first electromagnetic pulse. 12. The method of claim 1 , wherein the physical qubit comprises a Josephson junction. 13. The method of claim 12 , wherein the physical qubit is a superconducting transmon qubit. 14. The method of claim 1 , wherein the quantum mechanical oscillator is a radiation cavity. 15. The method of claim 14 , wherein the quantum mechanical oscillator is a microwave stripline cavity. 16. The method of claim 1 , wherein the first electromagnetic pulse comprises microwave frequencies. 17. A circuit quantum electrodynamics system, comprising: a physical qubit; a quantum mechanical oscillator dispersively coupled to the physical qubit; and at least one electromagnetic radiation source configured to independently apply electromagnetic pulses to the qubit and to the oscillator by: applying a first electromagnetic pulse to the physical qubit based on a number state of the quantum mechanical oscillator to cause a change in state of the quantum mechanical oscillator; and applying a second electromagnetic pulse to the quantum mechanical oscillator to coherently add or remove energy from the quantum mechanical oscillator. 18. The system of claim 17 , wherein: the quantum mechanical oscillator is a first quantum mechanical oscillator; the system further comprises a second quantum mechanical oscillator coupled to the physical qubit; and a quality factor of the second quantum mechanical oscillator is lower than a quality factor of the first quantum mechanical oscillator. 19. The system of claim 17 , wherein the change in state of the quantum mechanical oscillator caused by the first electromagnetic pulse is a quantum phase change of one or more Fock state components of the quantum mechanical oscillator. 20. The system of claim 17 , wherein a qubit frequency shift per photon in the quantum mechanical oscillator is larger than a qubit transition line width. 21. The system of claim 17 , wherein the first electromagnetic pulse includes a first frequency component and wherein the quantum mechanical oscillator is resonant at a second frequency, different from the first frequency. 22. The system of claim 17 , wherein the physical qubit comprises a Josephson junction. 23. The system of claim 22 , wherein the physical qubit is a superconducting transmon qubit. 24. The system of claim 17 , wherein the quantum mechanical oscillator is a radiation cavity. 25. The system of claim 24 , wherein the quantum mechanical oscillator is a microwave stripline cavity. 26. The system of claim 17 , wherein the first electromagnetic pulse is configured to comprise microwave frequencies.

Assignees

Inventors

Classifications

  • using superconductive devices · CPC title

  • the active element in the amplifier being a semiconductor device · CPC title

  • G06N10/00Primary

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

  • G06N10/40Primary

    Physical realisations or architectures of quantum processors or components for manipulating qubits, e.g. qubit coupling or qubit control · CPC title

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

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What does patent US10540602B2 cover?
According to some aspects, a method is provided of operating a circuit quantum electrodynamics system that includes a physical qubit dispersively coupled to a quantum mechanical oscillator, the method comprising applying a first electromagnetic pulse to the physical qubit based on a number state of the quantum mechanical oscillator, wherein the first electromagnetic pulse causes a change in sta…
Who is the assignee on this patent?
Univ Yale
What technology area does this patent fall under?
Primary CPC classification G06N10/00. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Jan 21 2020 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 7 related publications on this page (citations in our corpus or others sharing the same primary CPC).