Quantum D-state AC-Stark shift gate
A quantum computing D-state AC-Stark shift gate system comprises at least one gate manipulation source and one or more ions trapped in an ion trap. The at least one gate manipulation source is configured to generate a first gate manipulation signal and a second gate manipulation signal. The first and second gate manipulation signals couple an ion between a set of S-states and a set of D-states. The first and second gate manipulation signals apply a force to an ion of the one or more ions that is dependent on the internal state of the ion. The first and second gate manipulation signals are configured to couple internal states of the ions to their motional state without appreciably altering a population of the ions within the set of S-states.
1. A quantum computing D-state AC-Stark shift gate system comprising:
a first gate manipulation source configured to generate a first gate manipulation signal at a first laser wavelength;
a second gate manipulation source configured to generate a second gate manipulation signal at a second laser wavelength;
an ion trap; and
one or more ions trapped within the ion trap,
wherein the first gate manipulation signal is configured to couple a set of S-states and a set of D-states of the one or more ions,
wherein the second gate manipulation signal is configured to couple said set of S-states and said set of D-states of the one or more ions,
wherein a force applied to an ion of the one or more ions by the first and second gate manipulation signals is dependent on the internal state of the ion, and
wherein the first and second gate manipulation signals are configured to couple internal states of the one or more ions to their motional state without appreciably altering a population of the one or more ions within the set of S-states.
2. The system of claim 1 , wherein the system includes a magnetic field generating device configured to generate a magnetic field.
3. The system of claim 1 , wherein the second gate manipulation signal propagates in a direction not parallel to the first gate manipulation signal.
4. The system of claim 3 , wherein the second gate manipulation signal propagates in a direction approximately perpendicular to the first gate manipulation signal.
5. The system of claim 4 , wherein:
the first gate manipulation signal is polarized having a first orientation; and
the second gate manipulation signal is polarized having a second orientation substantially perpendicular to the first orientation;
wherein the polarizations lie within a plane defined by the propagation directions of the two gate manipulation signals.
6. The system of claim 4 , wherein:
the first gate manipulation signal is polarized in a plane having a first orientation; and
the second gate manipulation signal is polarized out of the plane having a second orientation substantially perpendicular to the first orientation;
wherein the plane is defined by the propagation directions of the two gate manipulation signals.
7. The system of claim 3 , wherein the second gate manipulation signal propagates in a direction approximately opposite to the first gate manipulation signal.
8. The system of claim 1 , wherein the second gate manipulation signal propagates in a direction approximately parallel to the first gate manipulation signal.
9. The system of claim 1 , wherein the first and second gate manipulation signals are modulations of a common gate manipulation signal.
10. The system of claim 1 , wherein the first gate manipulation source is configured to couple the ion off-resonantly between a subset of the S-states and a subset of the D-states and the second gate manipulation source is configured to couple the ion off-resonantly between said subset of S-states and said subset of D-states.
11. The system of claim 1 , wherein the first laser wavelength is a first visible spectrum laser wavelength, and the second laser wavelength is a second visible spectrum laser wavelength.
12. The system of claim 1 , wherein the first laser wavelength is a first infrared or ultra-violet spectrum laser wavelength, and the second laser wavelength is a second infrared or ultra-violet spectrum laser wavelength.
13. The system of claim 1 , wherein the first laser wavelength and the second laser wavelength are detuned outside a hyperfine manifold of the set of D-states.
14. The system of claim 1 , wherein the first laser wavelength and the second laser wavelength are detuned within a hyperfine manifold of the set of D-states.
15. The system of claim 14 , wherein the first laser wavelength and the second laser wavelength are detuned symmetrically within the hyperfine manifold of the set of D-states.
16. The system of claim 1 , wherein the first gate manipulation signal and the second gate manipulation signal include a pulse shaping modulation to reduce the population of the D-states upon completion of the gate operation.
17. The system of claim 16 , wherein the pulse shaping modulation includes a rise and fall modulation in the form sin 2 (t).
18. The system of claim 1 , wherein the one or more ions are ions that have a low-lying D-state.
19. The system of claim 18 , wherein the one or more ions comprise at least one of singly ionized ytterbium, singly ionized barium, singly ionized strontium, or singly ionized calcium.
20. A quantum computing D-state AC-Stark shift gate method comprising:
generating a first gate manipulation signal at a first laser wavelength using a first gate manipulation source, said first gate manipulation signal configured to couple a set of S-states of one or more ions trapped within an ion trap to a set of D-states of the one or more ions;
generating a second gate manipulation signal at a second laser wavelength using a second gate manipulation source, said second gate manipulation source configured to couple said set of S-states to said set of D-states of the one or more ions; and
applying said first gate manipulation signal and said second gate manipulation signal to the one or more ions,
wherein a force applied to an ion of the one or more ions by the first and second gate manipulation signals is dependent on the internal state of the ion, and
wherein the first and second gate manipulation signals are configured to couple internal states of the one or more ions to their motional state without appreciably altering a population of the one or more ions within the set of S-states.