Granted Patent B2

US 12,265,884 · App. 17/464,595 · Granted Apr 1, 2025

Inventors: Reinhold Blumel (Middletown, CT); Nikodem Grzesiak (College Park, MD); Ming Li (Silver Spring, MD); Andrii Maksymov (Hyattsville, MD); Yunseong Nam (North Bethesda, MD)

Assignee: IONQ, INC.

G06N10/20G06N10/40

Abstract

Claims (55)

1. A method for performing an entangling operation between trapped ions in a quantum computer, comprising:

selecting, by a classical computer, a gate duration of a pulse to be applied to two trapped ions in a quantum processor, comprising a plurality of trapped ions, wherein each of the trapped ions has two frequency-separated states defining a qubit, and the pulse is generated by one or more lasers;

selecting, by the classical computer, an amount of infidelity that is allowed in an entangling operation between the two trapped ions;

computing, by the classical computer, a first set of values of an amplitude and a detuning frequency of the pulse based on the selected gate duration, the selected amount of infidelity, and a phase-space condition for states of the plurality of trapped ions to remain unchanged at the end of the gate duration;

selecting, by the classical computer, a second set of values of the amplitude and the detuning frequency of the pulse among the first set of values based on a gate angle condition for entangling interaction between the two trapped ions to be a selected value;

generating, by the classical computer, the pulse based on the second set of values of the amplitude and the detuning frequency of the pulse;

applying, by use of a system controller and the one or more lasers, the generated pulse to each of the two trapped ions to perform the entangling operation between the two trapped ions;

measuring, by use of the system controller, a population of gubit states in the quantum processor; and

outputting, by the classical computer, the measured population of qubit states.

2. The method of claim 1 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse comprises decomposing a pulse function is decomposed of the pulse using basis functions, and computing coefficients of the basis functions.

3. The method of claim 2 , wherein the computing of the coefficients of the basis functions comprises:

selecting the coefficients of the basis functions such that infidelity of the entangling operation caused by a pulse having the pulse function equals the selected amount of infidelity.

4. The method of claim 2 , wherein the computing of the coefficients of the basis functions comprises:

selecting the coefficients of the basis functions from an extended solution space, in which the entangling operation caused by a pulse having the pulse function satisfies the phase-space condition and the gate angle condition within a predetermined threshold value.

5. The method of claim 1 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse is further based on stabilization conditions.

6. The method of claim 1 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse is further based on a power optimization condition.

7. An ion trap quantum computing system, comprising:

a quantum processor comprising a plurality of trapped ions, each trapped ion having two hyperfine states defining a qubit;

one or more lasers configured to emit a laser beam, which is provided to trapped ions in the quantum processor;

a classical computer configured to perform operations comprising:

selecting a gate duration of a pulse to be applied to two trapped ions in the quantum processor;

selecting an amount of infidelity that is allowed in an entangling operation between the two trapped ions;

computing a first set of values of an amplitude and a detuning frequency of the pulse based on the selected gate duration, the selected amount of infidelity, and a phase-space condition for states of the plurality of trapped ions to remain unchanged at the end of the gate duration;

selecting a second set of values of the amplitude and the detuning frequency of the pulse among the first set of values based on a gate angle condition for entangling interaction between the two trapped ions to be a selected value; and

generating the pulse based on the second set of values of the amplitude and the detuning frequency of the pulse; and

a system controller configured to execute a control program to control the one or more lasers to perform operations on the quantum processor, the operations comprising:

applying the generated pulse to each of the two trapped ions to perform the entangling operation between the two trapped ions; and

measuring population of qubit states in the quantum processor,

wherein the classical computer is further configured to output the measured population of qubit states in the quantum processor.

8. The ion trap quantum computing system of claim 7 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse comprises decomposing a pulse function of the pulse using basis functions, and computing coefficients of the basis functions.

9. The ion trap quantum computing system of claim 8 , wherein the computing of the coefficients of the basis functions comprises:

selecting the coefficients of the basis functions such that infidelity of the entangling operation caused by a pulse having the pulse function equals the selected amount of infidelity.

10. The ion trap quantum computing system of claim 8 , wherein the computing of the coefficients of the basis functions comprises:

selecting the coefficients of the basis functions from an extended solution space, in which the entangling operation caused by a pulse having the pulse function satisfies the phase-space condition and the gate angle condition within a predetermined threshold value.

11. The ion trap quantum computing system of claim 7 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse is further based on stabilization conditions.

12. The ion trap quantum computing system of claim 7 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse is further based on a power optimization condition.

13. An ion trap quantum computing system, comprising:

a classical computer;

a quantum processor comprising a plurality of trapped ions, each trapped ion having two hyperfine states defining a qubit;

a system controller configured to execute a control program to control one or more lasers to perform operations on the quantum processor; and

non-volatile memory having a number of instructions stored therein which, when executed by one or more processors, causes the ion trap quantum computing system to perform operations comprising:

selecting, by the classical computer, a gate duration of a pulse to be applied to two trapped ions in the quantum processor;

selecting, by the classical computer, an amount of infidelity that is allowed in an entangling operation between the two trapped ions;

computing, by the classical computer, a first set of values of an amplitude and a detuning frequency of the pulse to be applied to each of the two trapped ions based on the selected gate duration, the selected amount of infidelity, and a phase-space condition for states of the plurality of trapped ions to remain unchanged at the end of the gate duration;

selecting, by the classical computer, a second set of values of the amplitude and the detuning frequency of the pulse among the first set of values based on a gate angle condition for entangling interaction between the two trapped ions to be a selected value;

generating, by the classical computer, the pulse based on the second set of values of the amplitude and the detuning frequency of the pulse;

applying, by the system controller, the generated pulse to each of the two trapped ions to perform the entangling operation between the two trapped ions;

measuring, by the system controller, population of qubit states in the quantum processor; and

outputting, by the classical computer, the measured population of qubit states in the quantum processor.

14. The ion trap quantum computing system of claim 13 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse comprises decomposing a pulse function of the pulse using basis functions, and

selecting coefficients of the basis functions such that infidelity of the entangling operation caused by a pulse having the pulse function equals the selected amount of infidelity.

15. The ion trap quantum computing system of claim 13 , wherein computing the first set of values of the amplitude and the detuning frequency of the pulse comprises decomposing a pulse function of the pulse using basis functions, the computing of the pulse function comprises:

selecting coefficients of the basis functions from an extended solution space, in which the entangling operation caused by a pulse having the pulse function satisfies the phase-space condition and the gate angle condition within a predetermined threshold value.

16. The ion trap quantum computing system of claim 13 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse is further based on stabilization conditions.

17. The ion trap quantum computing system of claim 13 , wherein the computing of the first set of values of the amplitude and the detuning frequency of the pulse is further based on a power optimization condition.

Assignments (1)

Continuity (2)

References Cited (56)

Cited By (2)

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