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Exact Quantum Many-Body Scar States in the Rydberg-Blockaded Atom Chain

机译:Rydberg-Blockaded原子链中的精确量子多体疤痕态

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摘要

A recent experiment in the Rydberg atom chain observed unusual oscillatory quench dynamics with a charge density wave initial state, and theoretical works identified a set of many-body "scar states" showing nonthermal behavior in the Hamiltonian as potentially responsible for the atypical dynamics. In the same nonintegrable Hamiltonian, we discover several eigenstates at an infinite temperature that can be represented exactly as matrix product states with a finite bond dimension, for both periodic boundary conditions (two exact E = 0 states) and open boundary conditions (two E = 0 states and one each E = +/-root 2). This discovery explicitly demonstrates the violation of the strong eigenstate thermalization hypothesis in this model and uncovers exact quantum many-body scar states. These states show signatures of translational symmetry breaking with a period-2 bond-centered pattern, despite being in one dimension at an infinite temperature. We show that the nearby many-body scar states can be well approximated as "quasiparticle excitations" on top of our exact E = 0 scar states and propose a quasiparticle explanation of the strong oscillations observed in experiments.
机译:最近在Rydberg原子链上进行的一项实验观察到具有电荷密度波初始状态的异常振荡猝灭动力学,理论研究确定了一组多体“疤痕状态”,表明哈密顿量中的非热行为可能是非典型动力学的原因。 。在相同的不可积分哈密顿量中,我们发现了在无限大温度下的几个本征态,它们可以精确表示为具有有限键维的矩阵乘积态,对于周期边界条件(两个精确的E = 0状态)和开放边界条件(两个E = 0个状态,每个E = +/-根2)。该发现明确证明了该模型中强本征态热化假设的违反,并揭示了精确的量子多体疤痕状态。这些状态显示了平移对称性的特征,以2期键为中心的模式破裂,尽管在无限温度下处于一维状态。我们表明,在我们精确的E = 0疤痕状态之上,附近的多体疤痕状态可以很好地近似为“准粒子激发”,并提出了对实验中观察到的强振荡的准粒子解释。

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