# US 12,217,882 B2 · Methods and apparatuses for cross-talk mitigation

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- Number: US 12,217,882 B2
- Document ID: US12217882B2
- Status: Granted
- Kind: B2
- Application number: 17/867,414
- Filed: 2022-07-18
- Published: 2023-02-02
- Granted: 2025-02-04
- Earliest claimed: 2021-07-16
- Assignees: IonQ, Inc.
- Applicants: IonQ, Inc.
- Inventors: Michael Lurie Goldman; Jonathan Albert Mizrahi; Jeremy Matthew Sage
- Web page: https://patentgrep.com/patent/US12217882B2

## CPC

- G21K 1/20: for confining charged particles or handling confined charged particles, e.g. ion traps
- G06N 10/40: Physical realisations or architectures of quantum processors or components for manipulating qubits, e.g. qubit coupling or qubit control
- G06N 10/70: Quantum error correction, detection or prevention, e.g. surface codes or magic state distillation
- G21K: HANDLING OF PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G06N: COMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS

## Abstract

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.

## Claims

### Claim 1

A method for operating a quantum computer system, comprising:
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 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 to the metastable state.

### Claim 2 (depends on 1)

The method of claim 1, further comprising, prior to applying the at least first Raman beam and the at least second Raman beam:
applying each of a plurality of Raman beams to each corresponding trapped ion of the plurality of trapped ions; and
measuring optical cross-talk associated with neighboring trapped ions in response to applying each of the plurality of Raman beams to each of the corresponding trapped ion.

### Claim 3 (depends on 2)

The method of claim 2, further comprising:
selecting a first portion of the plurality of trapped ions, wherein first optical cross-talk of the first portion of the plurality of trapped ions is lower than second optical cross-talk of a second portion of the plurality of trapped ions.

### Claim 4 (depends on 3)

The method of claim 3, wherein the first portion of the plurality of trapped ions includes the at least two non-consecutive trapped ions.

### Claim 5 (depends on 1)

The method of claim 1, wherein applying the at least a first Raman beam comprises applying a composite pulse sequence.

### Claim 6 (depends on 1)

The method of claim 1, wherein the plurality of trapped ions includes a plurality of dual-space, single-species (DSSS) trapped-ions.

### Claim 7

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:
identify an ion chain having a plurality of trapped ions;
select at least two non-consecutive trapped ions in the ion chain for implementing a qubit;
cause a first light source to apply at least a first Raman beam to shuttle at least one neighbor of the at least two non-consecutive trapped ions from a ground state to a metastable state; and
cause a second light source to apply 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 to the metastable state.

### Claim 8 (depends on 7)

The non-transitory computer readable medium of claim 7, further comprises instructions for:
causing a third light source to apply each of a plurality of Raman beams to each corresponding trapped ion of the plurality of trapped ions; and
measuring optical cross-talk associated with neighboring trapped ions in response to applying each of the plurality of Raman beams to each of the corresponding trapped ion.

### Claim 9 (depends on 8)

The non-transitory computer readable medium of claim 8, further comprising instructions for:
selecting a first portion of the plurality of trapped ions, wherein first optical cross-talk of the first portion of the plurality of trapped ions is lower than second optical cross-talk of a second portion of the plurality of trapped ions.

### Claim 10 (depends on 9)

The non-transitory computer readable medium of claim 9, wherein the first portion of the plurality of trapped ions includes the at least two non-consecutive trapped ions.

### Claim 11 (depends on 7)

The non-transitory computer readable medium of claim 7, wherein the instructions for causing the first light source to apply the at least a first Raman beam comprises instructions for causing the first light source to apply a composite pulse sequence.

### Claim 12 (depends on 7)

The non-transitory computer readable medium of claim 7, wherein the plurality of trapped ions includes a plurality of dual-space, single-species (DSSS) trapped-ions.

### Claim 13

A quantum information processing (QIP) system, comprising:
a controller configured to:
identify an ion chain having a plurality of trapped ions;
select at least two non-consecutive trapped ions in the ion chain for implementing a qubit;
a first light source configured to apply at least a first Raman beam to shuttle at least one neighbor of the at least two non-consecutive trapped ions from a ground state to a metastable state; and
a second light source configured to apply 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 to the metastable state.

### Claim 14 (depends on 13)

The QIP system of claim 13, further comprising:
a third light source configured to apply each of a plurality of Raman beams to each corresponding trapped ion of the plurality of trapped ions; and
wherein the controller is further configured to measure optical cross-talk associated with neighboring trapped ions in response to applying each of the plurality of Raman beams to each of the corresponding trapped ion.

### Claim 15 (depends on 14)

The QIP system of claim 14, wherein the controller is further configured to select a first portion of the plurality of trapped ions, wherein first optical cross-talk of the first portion of the plurality of trapped ions is lower than second optical cross-talk of a second portion of the plurality of trapped ions.

### Claim 16 (depends on 15)

The QIP system of claim 15, wherein the first portion of the plurality of trapped ions includes the at least two non-consecutive trapped ions.

### Claim 17 (depends on 13)

The QIP system of claim 13, wherein the first light source is further configured to apply a composite pulse sequence.

### Claim 18 (depends on 13)

The QIP system of claim 13, wherein the plurality of trapped ions includes a plurality of dual-space, single-species (DSSS) trapped-ions.
