Methods and apparatuses for micromotion compensation with displaced beam

US12164072B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-12164072-B2
Application numberUS-202218050864-A
CountryUS
Kind codeB2
Filing dateOct 28, 2022
Priority dateJul 16, 2021
Publication dateDec 10, 2024
Grant dateDec 10, 2024

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  5. First independent claim

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Abstract

Official abstract text for this publication.

Aspects of the present disclosure may include a method and/or a system for identifying an ion chain having a plurality of trapped ions, selecting at least two non-consecutive trapped ions in the ion chain for implementing a qubit, applying at least a first Raman beam to shuttle at least one neighbor ion of the at least two non-consecutive trapped ions from a ground state to a metastable state, and applying at least a second Raman beam to one or more of the at least two non-consecutive trapped ions, after shuttling the at least one neighbor ion to the metastable state, to transition from a first manifold to a second manifold.

First claim

Opening claim text (preview).

What is claimed is: 1. A method of identifying micromotion in a quantum information processing (QIP) system, comprising: generating a Raman beam having a plurality of points associated with an intensity profile decreasing radially from at least a center point of the Raman beam; applying the Raman beam to a dual space single species (DSSS) trapped ion such that the DSSS trapped ion overlaps with a point of the plurality of points, wherein the point is not the center point of the Raman beam; applying a radio frequency (RF) field to the DSSS trapped ion to trap the DSSS trapped ion; applying a plurality of compensation fields to the DSSS trapped ion; measuring a plurality of micromotions of the DSSS trapped ion, wherein each respective micromotion is associated with a respective compensation field of the plurality of compensation fields; identifying at least one minimum micromotion of the plurality of micromotions; and identifying at least one compensation field that induces the at least one minimum micromotion. 2. The method of claim 1 , further comprising: applying the Raman beam to the DSSS trapped ion such that the DSSS trapped ion substantially overlaps with the center point; applying the at least one compensation field during a computation process to reduce the micromotion. 3. The method of claim 1 , further comprising applying a plurality of instances of the Raman beam, wherein each instance of the plurality of instances comprises applying the Raman beam to the DSSS trapped ion such that the DSSS trapped ion overlaps with a subset of the plurality of points. 4. The method of claim 3 , further comprising, for each instance of the Raman beam: applying a corresponding plurality of compensation fields to the DSSS trapped ion; measuring a corresponding plurality of micromotions of the DSSS trapped ion, wherein each respective micromotion is associated with a respective compensation field of the corresponding plurality of compensation fields; identifying a corresponding minimum micromotion of the corresponding plurality of micromotions; and identifying a corresponding compensation field that induces the corresponding minimum micromotion. 5. The method of claim 3 , wherein applying the plurality of instances of the Raman beam comprises applying the plurality of instances of the Raman beam without substantially altering a plurality of incident angles associated with the plurality of instances of the Raman beam. 6. A non-transitory computer readable medium having instructions stored therein that, when executed by one or more processors of a quantum information processing (QIP) system, cause the one or more processors to: generate a Raman beam having a plurality of points associated with an intensity profile decreasing radially from at least a center point of the Raman beam; apply the Raman beam to a dual space single species (DSSS) trapped ion such that the DSSS trapped ion overlaps with a point of the plurality of points, wherein the point is not the center point of the Raman beam; apply a radio frequency (RF) field to the DSSS trapped ion to trap the DSSS trapped ion; apply a plurality of compensation fields to the DSSS trapped ion; measure a plurality of micromotions of the DSSS trapped ion, wherein each respective micromotion is associated with a respective compensation field of the plurality of compensation fields; identify at least one minimum micromotion of the plurality of micromotions; and identify at least one compensation field that induces the at least one minimum micromotion. 7. The non-transitory computer readable medium of claim 6 , further comprising instructions for: applying the Raman beam to the DSSS trapped ion such that the DSSS trapped ion substantially overlaps with the center point; applying the at least one compensation field during a computation process to reduce the micromotion. 8. The non-transitory computer readable medium of claim 6 , further comprising instructions for applying a plurality of instances of the Raman beam, wherein each instance of the plurality of instances comprises applying the Raman beam to the DSSS trapped ion such that the DSSS trapped ion overlaps with a subset of the plurality of points. 9. The non-transitory computer readable medium of claim 8 , further comprising instructions, for each instance of the Raman beam: applying a corresponding plurality of compensation fields to the DSSS trapped ion; measuring a corresponding plurality of micromotions of the DSSS trapped ion, wherein each respective micromotion is associated with a respective compensation field of the corresponding plurality of compensation fields; identifying a corresponding minimum micromotion of the corresponding plurality of micromotions; and identifying a corresponding compensation field that induces the corresponding minimum micromotion. 10. The non-transitory computer readable medium of claim 8 , wherein the instructions for applying the plurality of instances of the Raman beam comprises instructions for applying the plurality of instances of the Raman beam without substantially altering a plurality of incident angles associated with the plurality of instances of the Raman beam. 11. A quantum information processing (QIP) system, comprising: a light source configured to: generate a Raman beam having a plurality of points associated with an intensity profile decreasing radially from at least a center point of the Raman beam; apply the Raman beam to a dual space single species (DSSS) trapped ion such that the DSSS trapped ion overlaps with a point of the plurality of points, wherein the point is not the center point of the Raman beam a power source configured to apply a radio frequency (RF) field to the DSSS trapped ion to trap the DSSS trapped ion; apply a plurality of compensation fields to the DSSS trapped ion a controller configured to: measure a plurality of micromotions of the DSSS trapped ion, wherein each respective micromotion is associated with a respective compensation field of the plurality of compensation fields; identify at least one minimum micromotion of the plurality of micromotions; and identify at least one compensation field that induces the at least one minimum micromotion. 12. The QIP system of claim 11 , wherein: the light source is further configured to apply the Raman beam to the DSSS trapped ion such that the DSSS trapped ion substantially overlaps with the center point; and the power source is further configured to apply the at least one compensation field during a computation process to reduce the micromotion. 13. The QIP system of claim 11 , wherein the light source is further configured to apply a plurality of instances of the Raman beam, wherein each instance of the plurality of instances comprises applying the Raman beam to the DSSS trapped ion such that the DSSS trapped ion overlaps with a subset of the plurality of points. 14. The QIP system of claim 13 , wherein, for each instance of the Raman beam: the power source is further configured to apply a corresponding plurality of compensation fields to the DSSS trapped ion; and the light source is further configured to: measure a corresponding plurality of micromotions of the DSSS trapped ion, wherein each respective micromotion is associated with a respective compensation field of the corresponding plurality of compensation fields; identify a corresponding minimum micromotion of the corresponding plurality of micromotions; and identify a corresponding compensation field that induces the corresponding minimum micromotion. 15. The QIP system of claim 13 , whe

Assignees

Inventors

Classifications

  • for confining charged particles or handling confined charged particles, e.g. ion traps · 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

  • G01T5/00Primary

    Recording of movements or tracks of particles (spark chambers H01J47/00); Processing or analysis of such tracks · CPC title

  • Physics · mapped topic

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What does patent US12164072B2 cover?
Aspects of the present disclosure may include a method and/or a system for identifying an ion chain having a plurality of trapped ions, selecting at least two non-consecutive trapped ions in the ion chain for implementing a qubit, applying at least a first Raman beam to shuttle at least one neighbor ion of the at least two non-consecutive trapped ions from a ground state to a metastable state, …
Who is the assignee on this patent?
Ionq Inc
What technology area does this patent fall under?
Primary CPC classification G06N10/40. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Dec 10 2024 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 5 related publications on this page (citations in our corpus or others sharing the same primary CPC).