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:
computing a first set of values of a first amplitude and a first detuning frequency of a first laser pulse to be applied to a first ion of an ion chain, and a second set of values of a second amplitude and a second detuning frequency of a second laser pulse to be applied to a second ion of the ion chain, the ion chain comprising a plurality of ions that are aligned in a first direction, each of the plurality of ions having two frequency-separated states defining a qubit, based on a condition for returning of the first and second ions in the ion chain to their original positions and momentum values without requiring a condition for non-zero entanglement interaction between the first and second ions;
selecting a third set of values of the first amplitude and the first detuning frequency among the first set of values, and a fourth set of values of the second amplitude and the second detuning frequency among the second set of values, based on the condition for non-zero entanglement interaction between the first and second ions;
selecting values of the first amplitude and the first detuning frequency among the third set of values, and values of the second amplitude and the second detuning frequency among the fourth set of values, based on a condition that variations of the non-zero entanglement interaction between the first and second ions with respect to fluctuations in frequencies of collective motional modes of the ion chain in a second direction that is perpendicular to the first direction are zero; and
applying the first laser pulse having the selected values of the first amplitude and the first detuning frequency to the first ion and the second laser pulse having the selected values of the second amplitude and the second detuning frequency to the second ion.
2. The method according to claim 1 , wherein
the computing of the first set of values and the second set of values is further based on a condition that variations of phase space trajectories of the first and second ions with respect to fluctuations in the frequencies of the collective motional modes of the ion chain in the second direction are zero.
3. The method according to claim 2 , wherein
the first amplitude is equal to the second amplitude, and
the first detuning frequency is equal to the second detuning frequency.
4. The method according to claim 2 , wherein
the first amplitude is different from the second amplitude, and
the first detuning frequency is different from the second detuning frequency.
5. The method according to claim 1 , wherein
the first amplitude is equal to the second amplitude, and
the first detuning frequency is equal to the second detuning frequency.
6. The method according to claim 1 , wherein
the first amplitude is different from the second amplitude, and
the first detuning frequency is different from the second detuning frequency.
7. The method according to claim 1 , wherein
the selecting of the values of the first amplitude and the first detuning frequency and the values of the second amplitude and the second detuning frequency is further based on power provided to the first and second ions by the first and second laser pulses.
8. The method according to claim 1 , further comprising:
modifying the first amplitude of the first laser pulse and the second amplitude of the second laser pulse such that the non-zero entanglement interaction between the first and second ions is calibrated to a predetermined value.
9. The method according to claim 1 , further applying a broadband laser pulse sequence to stabilize the non-zero entanglement interaction between the first and second ions when it is determined that a coupling strength of the first and second ions fluctuates with the collective motional modes.
10. A quantum computing system, comprising:
an ion chain comprising a plurality of ions that are aligned in a first direction, each of the ions having two hyperfine states defining a qubit; and
a controller comprising memory having a number of instructions stored therein which, when executed by a processor, causes the quantum computing system to perform operations comprising:
computing a first set of values of a first amplitude and a first detuning frequency of a first laser pulse to be applied to a first ion of an ion chain, and a second set of values of a second amplitude and a second detuning frequency of a second laser pulse to be applied to a second ion of the ion chain, based on a condition for returning of the first and second ions in the ion chain to their original positions and momentum values without requiring a condition for non-zero entanglement interaction between the first and second ions;
selecting a third set of values of the first amplitude and the first detuning frequency among the first set of values, and a fourth set of values of the second amplitude and the second detuning frequency among the second set of values, based on the condition for non-zero entanglement interaction between the first and second ions;
selecting values of the first amplitude and the first detuning frequency among the third set of values, and values of the second amplitude and the second detuning frequency among the fourth set of values, based on a condition that variations of the non-zero entanglement interaction between the first and second ions with respect to fluctuations in frequencies of collective motional modes of the ion chain in a second direction that is perpendicular to the first direction are zero; and
applying the first laser pulse having the selected values of the first amplitude and the first detuning frequency to the first ion and the second laser pulse having the selected values of the second amplitude and the second detuning frequency to the second ion.
11. The quantum computing system according to claim 10 , wherein each of the ions is 171 Yb + having the 2 S 1/2 hyperfine states.
12. The quantum computing system according to claim 10 , wherein
the computing of the first set of values and the second set of values is further based on a condition that variations of phase space trajectories of the first and second ions with respect to fluctuations in the frequencies of the collective motional modes of the ion chain in the second direction are zero.
13. The quantum computing system according to claim 10 , wherein
the first amplitude is equal to the second amplitude, and
the first detuning frequency is equal to the second detuning frequency.
14. The quantum computing system according to claim 10 , wherein
the first amplitude is different from the second amplitude, and
the first detuning frequency is different from the second detuning frequency.
15. The quantum computing system according to claim 10 , wherein
the selecting of the values of the first amplitude and the first detuning frequency and the values of the second amplitude and the second detuning frequency is further based on power provided to the first and second ions by the first and second laser pulses.
16. The quantum computing system according to claim 10 , wherein the operations further comprise:
modifying the first amplitude of the first laser pulse and the second amplitude of the second laser pulse such that the non-zero entanglement interaction between the first and second ions is calibrated to a predetermined value.
17. The quantum computing system according to claim 10 , wherein the operations further comprise:
applying a broadband laser pulse sequence to stabilize the non-zero entanglement interaction between the first and second ions when it is determined that a coupling strength of the first and second ions fluctuates with the collective motional modes.