Ph.D. Thesis - Physics
Ph.D. Thesis - Physics
Ph.D. Thesis - Physics
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Chapter 7<br />
Quantum simulation in<br />
surface-electrode elliptical ion<br />
traps<br />
As discussed at length in this thesis, two-dimensional arrays of trapped ions have great<br />
potential for a number of types of quantum simulations, most particularly for the simulation<br />
of spin frustration. We report in Ch. 5 that an array of individual microtraps, although<br />
appealing for its ability to generate an evenly-spaced array of ions, suffers major drawbacks<br />
in the interaction rate between neighboring trapped ions, whether considering motional<br />
coupling or the simulated spin-spin interaction rate. This motivates our present study of<br />
ion-ion interactions between ions in the same potential well that form a 2-D array through<br />
mutual Coulomb repulsion. In this case, the motional coupling rate is on the same order of<br />
magnitude as that in a linear ion trap with the same ion-ion spacing.<br />
In this chapter, we explore one example of an trap that creates a 2-D array of ions: a<br />
surface-electrode elliptical Paul trap. We choose the Paul trap approach in order to avoid the<br />
large Zeeman shifts and crystal rotation associated with Penning traps, as we did in Ch. 5.<br />
The surface-electrode geometry, as in Ch. 6, is beneficial for simplicity of microfabrication<br />
and eventual scaling down to microscopic sizes, if required. Prior to this work, the only<br />
2-D ion crystal prepared in a Paul trap had been in a linear trap. An added benefit of<br />
our elliptical trap approach is the ability, in principle, to apply magnetic field gradients<br />
to wires that reside in the plane of the trap electrodes, creating magnetic field gradients<br />
that can effect state-dependent forces in a manner similar to that proposed in Ref. [CW08],<br />
but with theoretically much stronger interaction rates. This is another advantage of the<br />
surface-electrode elliptical trap over other methods for generating a 2-D array of ions in the<br />
same potential well.<br />
A sensible objection to this technique is the existence of micromotion that cannot be<br />
compensated away and that affects every ion in the trap. The reason for this is that<br />
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