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arxiv: 2211.00653 · v1 · pith:WKF3B3XBnew · submitted 2022-11-01 · ❄️ cond-mat.quant-gas · cond-mat.stat-mech· cond-mat.str-el· hep-lat· quant-ph

Trimer quantum spin liquid in a honeycomb array of Rydberg atoms

classification ❄️ cond-mat.quant-gas cond-mat.stat-mechcond-mat.str-elhep-latquant-ph
keywords quantumspinrydbergatomsliquidtrimerarraycharacterized
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Quantum spin liquids are elusive but paradigmatic examples of strongly correlated quantum states that are characterized by long-range quantum entanglement. Recently, the direct signatures of a gapped topological $\mathbb{Z}_2$ spin liquid have been observed in a system of Rydberg atoms arrayed on the ruby lattice. Here, we illustrate the concrete realization of a fundamentally different class of spin liquids in a honeycomb array of Rydberg atoms. Exploring the quantum phase diagram of this system using both density-matrix renormalization group and exact diagonalization simulations, several density-wave-ordered phases are characterized and their origins explained. More interestingly, in the regime where third-nearest-neighbor atoms lie within the Rydberg blockade radius, we find a novel ground state -- with an emergent $\mathrm{U}(1)\times \mathrm{U}(1)$ local symmetry -- formed from superpositions of classical {\it trimer} configurations on the dual triangular lattice. The fidelity of this trimer spin liquid state can be enhanced via dynamical preparation, which we explain by a Rydberg-blockade-based projection mechanism associated with the smooth turnoff of the laser drive. Finally, we discuss the robustness of the trimer spin liquid phase under realistic experimental parameters and demonstrate that our proposal can be readily implemented in current Rydberg atom quantum simulators.

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  1. Order-by-disorder and emergent Kosterlitz-Thouless phase in triangular Rydberg array

    cond-mat.str-el 2023-02 unverdicted novelty 5.0

    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.