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Calculating Floquet states of large quantum systems: A parallelization strategy and its cluster implementation

机译:计算大量子系统的Floquet状态:并行化   战略及其集群实施

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摘要

We present a numerical approach to calculate non-equilibrium eigenstates of aperiodically time-modulated quantum system. The approach is based on the use ofa chain of single-step time-independent propagating operators. Each operator istime-specific and constructed by combining the Magnus expansion of thetime-dependent system Hamiltonian with the Chebyshev expansion of an operatorexponent. A construction of a unitary matrix of the Floquet operator, whichevolves a system state over the full modulation period, is performed bypropagating the identity matrix over the period. The independence of theevolutions of basis vectors makes the propagation stage suitable forimplementation on a parallel cluster. Once the propagation stage is completed,a routine diagonalization of the Floquet matrix is performed. Finally, anadditional propagation round, now with the eigenvectors as the initial states,allows to resolve the time-dependence of the Floquet states and calculate theircharacteristics. We demonstrate the accuracy and scalability of the algorithmby applying it to calculate the Floquet states of two quantum models, namely(i) a synthesized random-matrix Hamiltonian and (ii) a many-body Bose-Hubbarddimer, both of the size up to $10^4$ states.
机译:我们提出了一种数值方法来计算非周期时间调制量子系统的非平衡本征态。该方法基于单步时间无关的传播算子链的使用。每个算子是特定于时间的,并且通过结合时变系统哈密顿量的马格努斯展开和算子指数的切比雪夫展开来构造。 Floquet算子的unit矩阵的构造通过在整个周期内传播恒等矩阵来执行,该construction矩阵在整个调制周期内演化系统状态。基向量演化的独立性使传播阶段适合在并行集群上实现。一旦传播阶段完成,就对Floquet矩阵进行常规对角化。最后,现在以特征向量为初始状态的附加传播回合可以解决Floquet状态的时间相关性并计算其特征。通过将其应用于计算两个量子模型的Floquet状态,我们证明了该算法的准确性和可扩展性,即(i)合成的随机矩阵哈密顿量和(ii)多体Bose-Hubbarddimer,两者的大小均达到10美元^ 4 $状态。

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