Ph.D. Thesis - Physics
Ph.D. Thesis - Physics
Ph.D. Thesis - Physics
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Figure 7-13: Scaling of the J-coupling rates for all three directions as a function of the ion<br />
height in an elliptical trap, for the three concentric square rings wire configuration. The<br />
value for each direction will only hold if the projection of the electron spin is entirely along<br />
that direction; this would give an Ising-type interaction.<br />
Numerically, this is nicely verified. We apply the above scaling law to the secular<br />
frequencies, compute the mean ion-ion distance, and calculate the J coupling as a function<br />
of h, the height of the ion above the trap surface (calculation with respect to r0 would<br />
yield the same scaling). The highest coupling rate plotted here is 700 s −1 , which will be<br />
observable if the dominant decoherence rates are significantly lower than that.<br />
By contrast, the fields due to the rings produce a field gradient at the location of the<br />
ions with the form ∂ B<br />
∂xi<br />
∂Bˆx<br />
∂Bˆy ∂Bˆz<br />
= ∂x ˆx + ∂y ˆy + ∂z ˆz. We expect basically the same scaling law<br />
for the rings as for the triple-Z, due to the above arguments. However, the total interaction<br />
rates are different (and higher, overall). This is plotted in Fig. 7-15.<br />
7.3.2 Discussion<br />
The above results are but a small sample of the interactions that may be created with<br />
magnetic field gradients. Indeed, one appealing thing about this approach is the sheer<br />
variety of forces that may be created. The source of this freedom is the fact that the<br />
wires that create the gradients are separated from the source of the trapping potentials.<br />
Thus, the tight integration of wires and trapping electrodes proposed in Ref. [CW08] is not<br />
required. However, this greater flexibility in the global potentials does not come without a<br />
cost; individually switching interactions between individual pairs of ions is not possible.<br />
The methods presented in the section will apply the same state-dependent force to<br />
every ion in a 2-D crystal in an elliptical trap. These translate into Ising or Heisenberg<br />
Hamiltonians, depending on the experimenter’s choice. There remain two major questions:<br />
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