Demodulation and smoothing of amplitude, frequency, and phase modulated pulses for optimal implementation of entangling gates in ion trap quantum computers
Embodiments described herein are generally related to a method and a system for constructing and delivering a pulse to perform an entangling gate operation between two trapped ions during a quantum computation, and more specifically, to a method of demodulating and spline interpolating a pulse that can be practically implemented in the system while increasing the fidelity of the entangling gate operation, or the probability that at least two ions are in the intended qubit state(s) after performing the entangling gate operation between the two ions.
1. A method of performing a computation using a quantum computer, comprising:
computing a phase function and an amplitude function of a laser pulse to cause entangling interaction between a pair of trapped ions of a plurality of trapped ions, each of the plurality of trapped ions having two frequency-separated states defining a qubit;
smoothing the computed phase function of the laser pulse;
computing a detuning frequency function of the laser pulse based on the smoothed phase function of the laser pulse;
spline interpolating the computed detuning frequency function of the laser pulse; and
applying a pulse having the spline interpolated detuning frequency function and the amplitude function to the pair of trapped ions.
2. The method according to claim 1 , wherein the smoothing of the computed phase function of the laser pulse comprises computing a weighted average of the computed phase function of the laser pulse over a time interval.
3. The method according to claim 1 , wherein the computing of the detuning frequency function of the laser pulse comprises computing the time-derivative of the smoothed phase function.
4. The method according to claim 1 , wherein the computing of the phase function and the amplitude function of the laser pulse is based on the condition for returning of trapped ions to their original positions and momentum values and the condition for non-zero entangling interaction.
5. The method according to claim 4 , wherein the computing of the phase function and the amplitude function of the laser pulse is further based on the condition for stabilization.
6. The method according to claim 4 , wherein the computing of the phase function and the amplitude function of the laser pulse is further based on the condition for minimized power.
7. A non-transitory computer-readable medium including computer program instructions, which when executed by a processor, cause the processor to:
compute a phase function and an amplitude function of a laser pulse to cause entangling interaction between a pair of trapped ions of a plurality of trapped ions, each of the plurality of trapped ions having two frequency-separated states defining a qubit;
smooth the computed phase function of the laser pulse;
compute a detuning frequency function of the laser pulse based on the smoothed phase function of the laser pulse;
spline interpolate the computed detuning frequency function of the laser pulse; and
apply a laser pulse having the spline interpolated detuning frequency function and the amplitude function to the pair of trapped ions.
8. The non-transitory computer-readable medium according to claim 7 , wherein the smoothing of the computed phase function of the laser pulse comprises computing a weighted average of the computed phase function of the laser pulse over a time interval.
9. The non-transitory computer-readable medium according to claim 7 , wherein the computing of the detuning frequency function of the laser pulse comprises computing the time-derivative of the smoothed phase function.
10. The non-transitory computer-readable medium according to claim 7 , wherein the computing of the phase function and the amplitude function of the laser pulse is based on the condition for returning of trapped ions to their original positions and momentum values and the condition for non-zero entangling interaction.
11. The non-transitory computer-readable medium according to claim 10 , wherein the computing of the phase function and the amplitude function of the laser pulse is further based on the condition for stabilization.
12. The non-transitory computer-readable medium according to claim 10 , wherein the computing of the phase function and the amplitude function of the laser pulse is further based on the condition for minimized power.
13. A quantum computing system, comprising:
a plurality of trapped ions, 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:
computing a phase function and an amplitude function of a laser pulse to cause entangling interaction between a pair of trapped ions of the plurality of trapped ions;
smoothing the computed phase function of the laser pulse;
computing a detuning frequency function of the laser pulse based on the smoothed phase function of the laser pulse;
spline interpolating the computed detuning frequency function of the laser pulse; and
applying a laser pulse having the spline interpolated detuning frequency function and the amplitude function to the pair of trapped ions.
14. The quantum computing system according to claim 13 , wherein
each of the trapped ions is an ion having a nuclear spin and an electron spin such that a difference between the nuclear spin and the electron spin is zero.
15. The quantum computing system according to claim 14 , wherein
each of the trapped ions is an ion having a nuclear spin ½ and the 2 S 1/2 hyperfine states.
16. The quantum computing system according to claim 13 , wherein the smoothing of the computed phase function of the laser pulse comprises computing a weighted average of the computed phase function of the laser pulse over a time interval.
17. The quantum computing system according to claim 13 , wherein the computing of the phase function of the laser pulse comprises computing the time-derivative of the smoothed phase function.
18. The quantum computing system according to claim 13 , wherein the computing of the phase function and the amplitude function of the laser pulse is based on the condition for returning of trapped ions to their original positions and momentum values and the condition for non-zero entangling interaction.
19. The quantum computing system according to claim 18 , wherein the computing of the detuning frequency function and the amplitude function of the laser pulse is further based on the condition for stabilization.
20. The quantum computing system according to claim 18 , wherein the computing of the detuning frequency function and the amplitude function of the laser pulse is further based on the condition for minimized power.