Stabilization of entangling gates for trapped-ion quantum computers
A method of performing a computation using a quantum computer includes generating a first laser pulse and a second laser pulse to cause entanglement interaction between a first trapped ion and a second trapped ion of a plurality of trapped ions that are aligned in a first direction, each of the plurality of trapped ions having two frequency-separated states defining a qubit, and applying the generated first laser pulse to the first trapped ion and the generated second laser pulse to the second trapped ion. Generating the first laser pulse and the second laser pulse includes stabilizing the entanglement interaction between the first and second trapped ions against fluctuations in frequencies of collective motional modes of the plurality of trapped ions in a second direction that is perpendicular to the first direction.
1. A method of performing a computation using a quantum computer, comprising:
generating a first laser pulse and a second laser pulse to cause entanglement interaction between a first trapped ion and a second trapped ion of a plurality of trapped ions that are aligned in a first direction, each of the plurality of trapped ions having two frequency-separated states defining a qubit, wherein generating the first laser pulse and the second laser pulse comprises:
stabilizing the entanglement interaction between the first and second trapped ions against fluctuations in frequencies of collective motional modes of the plurality of trapped ions in a second direction that is perpendicular to the first direction; and
applying the generated first laser pulse to the first trapped ion and the generated second laser pulse to the second trapped ion.
2. The method according to claim 1 , wherein generating the first laser pulse and the second laser pulse further comprises:
stabilizing phase space trajectories of the first and second trapped ions against fluctuations in the frequencies of the collective motional modes of the plurality of trapped ions in the second direction.
3. The method according to claim 2 , wherein stabilizing the entanglement interaction between the first and second trapped ions and the phase space trajectories of the first and second trapped ions comprises:
adjusting a first amplitude and a first detuning frequency value of the first laser pulse, and a second amplitude and a second detuning frequency value of the second laser pulse based on variations of the entanglement interaction between the first and second trapped ions and the phase space trajectories of the first and second trapped ions with respect to fluctuations in the frequencies of the collective motional modes of the plurality of trapped ions in the second direction.
4. The method according to claim 3 , wherein
the first amplitude is equal to the second amplitude, and
the first detuning frequency value is equal to the second detuning frequency value.
5. The method according to claim 3 , wherein
the first amplitude is different from the second amplitude, and
the first detuning frequency value is different from the second detuning frequency value.
6. The method according to claim 3 , wherein
the first amplitude and the first detuning frequency value of the first laser pulse, and the second amplitude and the second detuning frequency value of the second laser pulse are adjusted further based on power provided to the first and second trapped ions by the first and second laser pulses.
7. The method according to claim 3 , further comprising:
modifying the first amplitude of the first laser pulse and the second amplitude of the second laser pulse to calibrate the entanglement interaction between the first and second trapped ions when it is determined that intensities of the first and second laser pulses fluctuate.
8. The method according to claim 1 , further applying a broadband laser pulse sequence to stabilize the entanglement interaction between the first and second trapped ions when it is determined that a coupling strength of the first and second trapped ions fluctuates with the collective motional modes.
9. A non-transitory computer-readable medium including computer program instructions, which when executed by a processor, cause the processor to:
generate a first laser pulse and a second laser pulse to cause entanglement interaction between a first trapped ion and a second trapped ion of a plurality of trapped ions that are aligned in a first direction, each of the plurality of trapped ions having two frequency-separated states defining a qubit, wherein generating the first laser pulse and the second laser pulse comprises:
stabilizing the entanglement interaction between the first and second trapped ions against fluctuations in frequencies of collective motional modes of the plurality of trapped ions in a second direction that is perpendicular to the first direction; and
apply the generated first laser pulse to the first trapped ion and the generated second laser pulse to the second trapped ion.
10. The non-transitory computer-readable medium according to claim 9 , wherein generating the first laser pulse and the second laser pulse further comprises:
stabilizing phase space trajectories of the first and second trapped ions against fluctuations in the frequencies of the collective motional modes of the plurality of trapped ions in the second direction.
11. The non-transitory computer-readable medium according to claim 10 , wherein stabilizing the entanglement interaction between the first and second trapped ions and the phase space trajectories of the first and second trapped ions comprises:
adjusting a first amplitude and a first detuning frequency value of the first laser pulse, and a second amplitude and a second detuning frequency value of the second laser pulse based on variations of the entanglement interaction between the first and second trapped ions and the phase space trajectories of the first and second trapped ions with respect to fluctuations in the frequencies of the collective motional modes of the plurality of trapped ions in the second direction.
12. The non-transitory computer-readable medium according to claim 11 , wherein
the first amplitude is equal to the second amplitude, and
the first detuning frequency value is equal to the second detuning frequency value.
13. The non-transitory computer-readable medium according to claim 11 , wherein
the first amplitude is different from the second amplitude, and
the first detuning frequency value is different from the second detuning frequency value.
14. The non-transitory computer-readable medium according to claim 11 , wherein
the first amplitude and the first detuning frequency value of the first laser pulse, and the second amplitude and the second detuning frequency value of the second laser pulse are adjusted further based on power provided to the first and second trapped ions by the first and second laser pulses.
15. The non-transitory computer-readable medium according to claim 11 , wherein the computer program instructions further cause the processor to:
modify the first amplitude of the first laser pulse and the second amplitude of the second laser pulse to calibrate the entanglement interaction between the first and second trapped ions when it is determined that intensities of the first and second laser pulses fluctuate.
16. The non-transitory computer-readable medium according to claim 9 , wherein the computer program instructions further cause the processor to:
apply a broadband laser pulse sequence to stabilize the entanglement interaction between the first and second trapped ions when it is determined that a coupling strength of the first and second trapped ions fluctuates with the collective motional modes.
17. A quantum computing system, comprising:
a plurality of trapped ions that are aligned in a first direction, each of the trapped ions having two hyperfine states defining a qubit; and
a controller comprising non-volatile memory having a number of instructions stored therein which, when executed by a processor, causes the quantum computing system to perform operations comprising:
generating a first laser pulse and a second laser pulse to cause entanglement interaction between a first trapped ion and a second trapped ion of the plurality of trapped ions, wherein generating the first laser pulse and the second laser pulse comprises:
stabilizing the entanglement interaction between the first and second trapped ions against fluctuations in frequencies of collective motional modes of the plurality of trapped ions in a second direction that is perpendicular to the first direction; and
applying the generated first laser pulse to the first trapped ion and the generated second laser pulse to the second trapped ion.
18. The quantum computing system according to claim 17 , wherein each of the trapped ions is 171 Yb + having the 2 S 1/2 hyperfine states.
19. The quantum computing system according to claim 17 , wherein generating the first laser pulse and the second laser pulse further comprises:
stabilizing phase space trajectories of the first and second trapped ions against fluctuations in the frequencies of the collective motional modes of the plurality of trapped ions in the second direction.
20. The quantum computing system according to claim 19 , wherein stabilizing the entanglement interaction between the first and second trapped ions and the phase space trajectories of the first and second trapped ions comprises:
adjusting a first amplitude and a first detuning frequency value of the first laser pulse, and a second amplitude and a second detuning frequency value of the second laser pulse based on variations of the entanglement interaction between the first and second trapped ions and the phase space trajectories of the first and second trapped ions with respect to fluctuations in the frequencies of the collective motional modes of the plurality of trapped ions in the second direction.
21. The quantum computing system according to claim 20 , wherein
the first amplitude is equal to the second amplitude, and
the first detuning frequency value is equal to the second detuning frequency value.
22. The quantum computing system according to claim 20 , wherein
the first amplitude is different from the second amplitude, and
the first detuning frequency value is different from the second detuning frequency value.
23. The quantum computing system according to claim 20 , wherein
the first amplitude and the first detuning frequency value of the first laser pulse, and the second amplitude and the second detuning frequency value of the second laser pulse are adjusted further based on power provided to the first and second trapped ions by the first and second laser pulses.
24. The quantum computing system according to claim 20 , wherein the operations further comprise:
modifying the first amplitude of the first laser pulse and the second amplitude of the second laser pulse to calibrate the entanglement interaction between the first and second trapped ions when it is determined that intensities of the first and second laser pulses fluctuate.
25. The quantum computing system according to claim 17 , wherein the operations further comprise:
applying a broadband laser pulse sequence to stabilize the entanglement interaction between the first and second trapped ions when it is determined that a coupling strength of the first and second trapped ions fluctuates with the collective motional modes.