Giachetti Guido, Defenu Nicolò
SISSA and INFN Sezione di Trieste, Via Bonomea 265, 34136, Trieste, Italy.
Institut für Theoretische Physik, ETH Zürich, Wolfgang-Pauli-Str. 27, Zurich, Switzerland.
Sci Rep. 2023 Jul 31;13(1):12388. doi: 10.1038/s41598-023-37984-3.
The prominent collective character of long-range interacting quantum systems makes them promising candidates for quantum technological applications. Yet, lack of additivity overthrows the traditional picture for entanglement scaling and transport, due to the breakdown of the common mechanism based on excitations propagation and confinement. Here, we describe the dynamics of the entanglement entropy in many-body quantum systems with a diverging contribution to the internal energy from the long-range two body potential. While in the strict thermodynamic limit entanglement dynamics is shown to be suppressed, a rich mosaic of novel scaling regimes is observed at intermediate system sizes, due to the possibility to trigger multiple resonant modes in the global dynamics. Quantitative predictions on the shape and timescales of entanglement propagation are made, paving the way to the observation of these phases in current quantum simulators. This picture is connected and contrasted with the case of local many body systems subject to Floquet driving.
长程相互作用量子系统显著的集体特性使其成为量子技术应用的理想候选者。然而,由于基于激发传播和限制的常见机制失效,缺乏可加性颠覆了传统的纠缠标度和传输图景。在这里,我们描述了多体量子系统中纠缠熵的动力学,其中长程两体势对内能的贡献发散。虽然在严格的热力学极限下,纠缠动力学被证明受到抑制,但在中等系统规模下,由于在全局动力学中触发多个共振模式的可能性,观察到了丰富多样的新型标度 regime。对纠缠传播的形状和时间尺度进行了定量预测,为在当前量子模拟器中观察这些相铺平了道路。这一图景与受弗洛凯驱动的局域多体系统的情况相联系并形成对比。