Ph.D. Thesis - Physics
Ph.D. Thesis - Physics
Ph.D. Thesis - Physics
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Figure 7-12: The triple-Z wire configuration and resulting magnetic fields. The wire configuration<br />
is top left; each wire carries 1A of current in the same direction. Each other<br />
the other plots gives the magnetic field components along a given direction. In all figures,<br />
Bˆx is in blue, Bˆy is in green, and Bˆz is in red. Note that the field gradients are quite<br />
constant across the volume occupied by the ions. Nonzero fields at the trap center must be<br />
cancelled by additional pairs of Helmholtz coils to avoid unwanted Zeeman shifts, electron<br />
alignments, and even ion crystal rotation.<br />
be operated at cryogenic temperatures suggests that superconducting wires could be used,<br />
mitigating resistive heating [REL + 08].<br />
We focus on two different wire configurations to give a flavor of the possibilities for<br />
simulated Hamiltonians. The first is a “Z” shape, the classic shape of the gradients coils<br />
used in chip-based atom traps. This shape is repeated three times, in order to further<br />
strengthen the field gradients. The second configuration is a set of three concentric square<br />
rings, that produce a different set of gradients.<br />
Results from the Z shape are given in Fig. 7-12. These are based on an elliptical trap<br />
that gives an ion height of 100 µm. We see that the gradient is of the approximate form<br />
∂ B<br />
∂xi<br />
= ∂Bˆz<br />
∂x<br />
ˆz + ∂Bˆz<br />
∂y<br />
∂Bˆx<br />
∂Bˆy<br />
ˆy + ∂z ˆz + ∂z ˆz. Depending on the projection of the atomic dipole, as set<br />
by the external bias fields, this yields the possibility of an Ising of Heisenberg interaction.<br />
The specific interaction induced depends upon the direction along which F acts.<br />
We now wish to calculate the actual interaction strengths and how they scale with the<br />
trap size. What do we expect? First, we recall from Ch. 5 that for constant trap depth<br />
the secular frequencies scale as 1/r0, where r0 is some characteristic length scale of the<br />
trap (usually defined as the distance from the ion to the rf electrode). At the same time,<br />
the distance between ions d is given by d 3 = e 2 c/(4πǫ0mω 2 ), as calculated by balancing the<br />
Coulomb and trapping forces. The magnetic field strengths scale as 1/r2 0 , and plugging that<br />
all into the formula for J (J ∝ F 2 /(ω4d3 )), we expect that J will scale as 1/r2 0 .<br />
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