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Bulletin of the American Physical Society

A compact room temperature trapped ion system

Yuhi Aikyo, Geert Vrijsen, Thomas Noël, Jungsang Kim

Published Mar 2, 2020• 0 citations
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Trapped Ion Temperature

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We present the design and vacuum performance of a compact room-temperature trapped ion system for quantum computing, consisting of an ultra-high vacuum (UHV) package, a micro-fabricated surface trap, and a small form-factor ion pump. The system is designed to maximize mechanical stability and robustness by minimizing the system size and weight. The internal volume of the UHV package is only ≈2 cm3, a significant reduction in comparison with conventional vacuum chambers used in trapped ion experiments. We demonstrate trapping of 174Yb+ ions in this system and characterize the vacuum level in the UHV package by monitoring both the rates of ion hopping in a double-well potential and ion chain reordering events. The calculated pressure in this vacuum package is ≈2.2×1011 Torr, which is sufficient for the majority of current trapped ion experiments.
We demonstrate coupling between the motions of two independently trapped ions with a separation distance of 620 μm. The ion-ion interaction is enhanced via a room-temperature electrically floating metallic wire which connects two surface traps. Tuning the motion of both ions into resonance, we show flow of energy with a coupling rate of 11 Hz. Quantum-coherent coupling is hindered by strong surface electric-field noise in our device. Our ion-wire-ion system demonstrates that room-temperature conductors can be used to mediate and tune interactions between independently trapped charges over distances beyond those achievable with free-space dipole-dipole coupling. This technology may be used to sympathetically cool or entangle remotely trapped charges and enable coupling between disparate physical systems.
We present a room-temperature Extreme High Vacuum (XHV) system engineered to support the long-duration operation of a trapped-ion quantum processor. Background-gas collisions impose limitations on trapped-ion performance and scalability by interrupting algorithmic execution and, in some cases, ejecting ions from the trap. Using molecular-flow simulations, we optimize the chamber geometry, conductance pathways, and pumping configuration to maximize the effective pumping speed at the ion location. We perform high-temperature heat treatment of stainless steel vacuum components to achieve the desired outgassing rate, guided by quantitative relations of bulk diffusive processes, allowing us to reduce the H2\mathrm{H_2}H2​ outgassing load to the 10−15 mbar l s−1 cm−210^{-15}\,\mathrm{mbar\,l\,s^{-1}\,cm^{-2}}10−15mbarls−1cm−2 level. The final pressure in our chamber, measured by a hot cathode gauge, is 1.5×10−12 mbar1.5\times10^{-12}\,\mathrm{mbar}1.5×10−12mbar, corresponding to the gauge's measurement limit. We measure the local pressure at the ion location by observing collision-induced reordering events in a long ion chain of mixed-isotope Yb+^++. From the observed reordering frequency, we extract the average interval between collisions to be (1.9±0.1) hrs/ion(1.9 \pm 0.1)\,\mathrm{hrs/ion}(1.9±0.1)hrs/ion. This corresponds to a local pressure of (3.9±0.3)×10−12 mbar(3.9 \pm 0.3)\times10^{-12}\,\mathrm{mbar}(3.9±0.3)×10−12mbar at the ion location, assuming that all collisions arise from background H2_22​ molecules at room temperature. Our demonstration extends the continuous operation time of a quantum processor while maintaining the simplicity of a room-temperature system that does not require cryogenic apparatus.