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非可积弗洛凯量子电路中的稳健有效基态

Robust Effective Ground State in a Nonintegrable Floquet Quantum Circuit.

作者信息

Ikeda Tatsuhiko N, Sugiura Sho, Polkovnikov Anatoli

机构信息

<a href="https://ror.org/02tt21044">RIKEN Center for Quantum Computing</a>, Wako, Saitama 351-0198, Japan.

Department of Physics, <a href="https://ror.org/05qwgg493">Boston University</a>, Boston, Massachusetts 02215, USA.

出版信息

Phys Rev Lett. 2024 Jul 19;133(3):030401. doi: 10.1103/PhysRevLett.133.030401.

DOI:10.1103/PhysRevLett.133.030401
PMID:39094155
Abstract

An external periodic (Floquet) drive is believed to bring any initial state to the featureless infinite temperature state in generic nonintegrable isolated quantum many-body systems in the thermodynamic limit, irrespective of the driving frequency Ω. However, numerical or analytical evidence either proving or disproving this hypothesis is very limited and the issue has remained unsettled. Here, we study the initial state dependence of Floquet heating in a nonintegrable kicked Ising chain of length up to L=30 with an efficient quantum circuit simulator, showing a possible counterexample: the ground state of the effective Floquet Hamiltonian is exceptionally robust against heating, and could stay at finite energy density even after infinitely many Floquet cycles, if the driving period is shorter than a threshold value. This sharp energy localization transition or crossover does not happen for generic excited states. The exceptional robustness of the ground state is interpreted by (i) its isolation in the energy spectrum and (ii) the fact that those states with L-independent ℏΩ energy above the ground state energy of any generic local Hamiltonian, like the approximate Floquet Hamiltonian, are atypical and viewed as a collection of noninteracting quasiparticles. Our finding paves the way for engineering Floquet protocols with finite driving periods realizing long-lived, or possibly even perpetual, Floquet phases by initial state design.

摘要

人们认为,在热力学极限下,对于一般的非可积孤立量子多体系统,外部周期性(弗洛凯)驱动会将任何初始状态带到无特征的无限温度状态,而与驱动频率Ω无关。然而,证明或反驳这一假设的数值或分析证据非常有限,这个问题一直没有得到解决。在这里,我们使用高效的量子电路模拟器研究了长度达L = 30的非可积踢伊辛链中弗洛凯加热对初始状态的依赖性,给出了一个可能的反例:如果驱动周期短于一个阈值,有效弗洛凯哈密顿量的基态对加热异常稳健,即使经过无限多个弗洛凯循环也能保持有限的能量密度。这种尖锐的能量局域化转变或交叉对于一般的激发态不会发生。基态的异常稳健性可由以下两点解释:(i)它在能谱中的孤立性;(ii)任何一般局域哈密顿量(如近似弗洛凯哈密顿量)的基态能量之上具有与L无关的ħΩ能量的那些状态是非典型的,可视为非相互作用准粒子的集合。我们的发现为通过初始状态设计来设计具有有限驱动周期的弗洛凯协议铺平了道路,这些协议可实现长寿命甚至可能是永久的弗洛凯相。

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