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Tunable Confinement-Deconfinement Transition in an Ultracold Atom Quantum Simulator

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arxiv 2204.06586 v1 pith:WIKH5TNO submitted 2022-04-13 cond-mat.quant-gas cond-mat.stat-mechcond-mat.str-elhep-lathep-th

Tunable Confinement-Deconfinement Transition in an Ultracold Atom Quantum Simulator

classification cond-mat.quant-gas cond-mat.stat-mechcond-mat.str-elhep-lathep-th
keywords modelchargeconfinementdeconfinementfixedgaugeangleatom
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The one-dimensional lattice Schwinger model has recently been realized by using bosons in optical lattices. This model contains both confinement and deconfinement phases, whose phase diagram is controlled by the mass of the matter field and the topological angle. Since varying the mass of matter field is straightforward experimentally, we propose how to tune the topological angle, allowing accessing the entire phase diagram. We propose that direct experimental evidence of confinement and deconfinement can be obtained by measuring whether a physical charge is localized around a fixed gauge charge to screen it. We also discuss the PXP model realized in the Rydberg atoms array, which is equivalent to the lattice Schwinger model when all local gauge charges are fixed as zero. Although the gauge charges are fixed, we can alternatively probe the confinement and the deconfinement in the PXP model by studying the relative motion of a pair of a physical charge and an anti-charge. Our scheme can be directly implemented in these two relevant experimental platforms of ultracold atom quantum simulators.

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    Numerical simulations of the Rydberg triangular lattice model show order-by-disorder √3×√3 order at half filling and an emergent KT phase at finite temperature.