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Ph.D. Thesis - Physics

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Figure 6-12: Measured pickup from the rf electrode during laser ablation. The rf begins<br />

recovering after about 15 µs, and during this time ions are trapped. Figure reproduced<br />

from Ref. [HMO + 06].<br />

lowered, some ions enter the trap, which returns to full strength with some ions already<br />

inside it. This was first observed by Hashimoto et al. [HMO + 06], and the relevant plot from<br />

that paper is presented in Fig. 6-12. The loading of ions into a conservative trap potential<br />

requires a nonconservative step; normally, it is the conversion of neutral atoms into ions<br />

within the trap, but with ablation loading it is an induced time-dependence of the trapping<br />

potentials themselves. We note also that lower-energy ablation pulses have been used in lieu<br />

of an oven to produce neutral atoms that are then photoionized within the trap [HGH + 07].<br />

Laser ablation has a number of possible advantages. For one, it requires only a single<br />

laser, and the process is not sensitive to its frequency. For instance, if one wished to load<br />

simultaneously atomic and molecular ions, an ablation pulse (or set of synchronized ablation<br />

pulses) might do the trick. As with e-gun loading, however, the lack of isotopic selection<br />

could potentially lead to unwanted trapped species. Second, it is very fast: carefully-<br />

calibrated ablation loading could thus be very useful for loading the many ions needed in<br />

a scalable quantum simulator. If an ion was lost during a simulation, one could envision<br />

a classical subroutine that pauses execution of the algorithm and then reloads an ion in<br />

the correct spot using a single ablation pulse. The ion could be trapped and re-cooled<br />

in much less than one second. Third, ablation loading does not create a large heat load.<br />

In a cryogenic environment, the heat generated by a resistive oven could be conducted to<br />

the trap electrodes, increasing decoherence rates. In our later work, we solve this problem<br />

by placing the oven in contact with the 40 K radiation shield, which has enough cooling<br />

power to handle the heat load. In the future, however, it may be advantageous to have very<br />

site-specific loading, as in the scenario described above. In this case, ablation loading may<br />

be a superb option.<br />

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