2022
DOI: 10.48550/arxiv.2204.06586
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Tunable Confinement-Deconfinement Transition in an Ultracold Atom Quantum Simulator

Abstract: 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 o… Show more

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Cited by 5 publications
(8 citation statements)
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“…Besides, by integrating versatile controllable tight-focused optical traps [38,39], we can also perform local measurements on individual atoms along different axes, satisfying the essential request of MBQC. More generally, our platform can offer new opportunities for quantum simulation of intriguing physics in lattice gauge theories [40][41][42][43][44] and exotic quantum phases in the quantum magnetism realm [45]. The capability on realizing low-entropy atom arrays together with the high-precision manipulation of single atoms may open the avenue to demonstrating practical quantum advantage [46].…”
Section: Discussionmentioning
confidence: 99%
“…Besides, by integrating versatile controllable tight-focused optical traps [38,39], we can also perform local measurements on individual atoms along different axes, satisfying the essential request of MBQC. More generally, our platform can offer new opportunities for quantum simulation of intriguing physics in lattice gauge theories [40][41][42][43][44] and exotic quantum phases in the quantum magnetism realm [45]. The capability on realizing low-entropy atom arrays together with the high-precision manipulation of single atoms may open the avenue to demonstrating practical quantum advantage [46].…”
Section: Discussionmentioning
confidence: 99%
“…For a related work, see Ref. [95], posted to the arXiv on the same day. τ = 0, and then steadily decreases during the ramp, approaching close to zero at its end (τ = 20 ms), where the system is deep in the Z 2 symmetry-broken phase.…”
Section: Discussionmentioning
confidence: 99%
“…The |Z 2 state also has large overlap with the scar states, preventing it from thermalization [33][34][35]. The PXP model is equivalent to this LGT model under the local gauge constraints of G l = 0 for all l, and therefore, the discussion also applies to this LGT model [16,36]. In Fig.…”
Section: One Potential Advantage Of Quantum Simulation For Studyingmentioning
confidence: 96%
“…In the near future, when our system size is enlarged several times, it will be beyond the capability of exact diagonalization. The experimental control and detection capability developed in this work can be used to study other interesting dynamical phenomena in this system, such as string breaking [37,38], dynamical transition between quantum phases [39,40], the false vacuum decay, and the confinement-deconfinement transition [16,36,41]. The current scheme of implementing the LGT can also be extended to higher dimensions [42].…”
Section: One Potential Advantage Of Quantum Simulation For Studyingmentioning
confidence: 99%