2021
DOI: 10.48550/arxiv.2112.00991
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An optical tweezer array of ground-state polar molecules

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Cited by 5 publications
(6 citation statements)
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“…Because one of the most widely-used schemes to create ultracold molecules is association of the constituent atoms [37][38][39], atoms are a readily available resource in many molecule experiments, making this scheme feasible to implement. As a concrete example, for a system of NaCs molecules and Cs atoms in optical tweezers [40], we show that sub-microsecond two-qubit gate times can be realized with high fidelity and at an interparticle spacing of 1 micron. We also outline a molecular detection scheme and avenues to extend the system to larger arrays, leveraging the mobility of optical tweezers and the many internal states of molecules.…”
Section: Introductionmentioning
confidence: 95%
“…Because one of the most widely-used schemes to create ultracold molecules is association of the constituent atoms [37][38][39], atoms are a readily available resource in many molecule experiments, making this scheme feasible to implement. As a concrete example, for a system of NaCs molecules and Cs atoms in optical tweezers [40], we show that sub-microsecond two-qubit gate times can be realized with high fidelity and at an interparticle spacing of 1 micron. We also outline a molecular detection scheme and avenues to extend the system to larger arrays, leveraging the mobility of optical tweezers and the many internal states of molecules.…”
Section: Introductionmentioning
confidence: 95%
“…However, the smaller contrast between high and low detection rates causes the transmission method to be generically slower than the fluorescence method of detection. Transmission measurements with a higher C would be interaction-free [33], thus suppressing depumping errors and mechanical effects from light scattering, which provides particular advantages for detecting trapped particles, such as single molecules [34,35], that lack a cycling optical transition.…”
mentioning
confidence: 99%
“…Here we resolve these problems, proposing how to scalably prepare a broad range of long-range entangled states with the use of existing experimental platforms. Our two-step process finds an ideal implementation in Rydberg atom arrays [11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26], only requiring time-evolution under the intrinsic atomic interactions, followed by measuring a single sublattice (by using, e.g., two atom species [27][28][29][30]). Remarkably, this protocol can prepare the 1D Greenberger-Horne-Zeilinger (GHZ) 'cat' state and 2D toric code [31] with fidelity per site exceeding 0.9999, and a 3D fracton state [32][33][34] with fidelity 0.998.…”
mentioning
confidence: 99%
“…While cluster states are already of interest (serving as resources for measurementbased quantum computation [47]), to produce long-range entanglement we need to be able to measure only a subsystem of its atoms. Recent breakthrough experiments have established that this is possible in dual-species arrays [27][28][29][30][48][49][50], where one species is transparent to measurements of the other. This way, we produce the 1D GHZ, the 2D toric code and 3D fracton states.…”
mentioning
confidence: 99%