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arXiv 2007.11174quant-phcond-mat.dis-nncond-mat.stat-mechmath-phmath.MP
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量子Gibbs态的改进热面积定律和准线性时间算法

Improved thermal area law and quasi-linear time algorithm for quantum Gibbs states

Tomotaka Kuwahara, Álvaro M. Alhambra, Anurag Anshu

摘要:

量子多体物理中最基本的问题之一是热态之间关联的表征。特别相关的是热面积法,它证明张量网络近似的热状态与键尺寸增长的多项式与系统的大小。在足够低的温度下,这是特别重要的实际应用,现有的技术不产生最佳的界限。在这里,我们提出了一个新的热面积法,适用于一般的多体系统的晶格。我们改进的温度依赖性从原来的$\mathcal{O}(β)$到$\tilde{\mathcal{O}}(β^{2/3})$,从而建议扩散传播的纠缠虚时间演化。这与通常导致纠缠线性增长的实时演化有质的不同。我们还证明了类似的限制的Rényi纠缠的净化和纠缠的形成。我们的分析是基于一个多项式近似的指数函数,它提供了一个时间演化和随机游动之间的关系。此外,对于一维(1D)系统的$n$自旋,我们证明了吉布斯状态是很好的近似与一个矩阵乘积算子的次线性键维数为$e^{\sqrt{\tilde{\mathcal{O}}(β\log(n))}}$。这个证明使我们能够严格地建立,第一次,一个准线性时间经典算法,用于构建一个MPS表示的一维量子吉布斯态在任意温度的$β= o(\log(n))$。我们的新技术成分是吉布斯状态的块分解,这与Haah等人给出的实时演化的分解相似,FOCS'18。

英文摘要:

One of the most fundamental problems in quantum many-body physics is the characterization of correlations among thermal states. Of particular relevance is the thermal area law, which justifies the tensor network approximations to thermal states with a bond dimension growing polynomially with the system size. In the regime of sufficiently low temperatures, which is particularly important for practical applications, the existing techniques do not yield optimal bounds. Here, we propose a new thermal area law that holds for generic many-body systems on lattices. We improve the temperature dependence from the original $\mathcal{O}(β)$ to $\tilde{\mathcal{O}}(β^{2/3})$, thereby suggesting diffusive propagation of entanglement by imaginary time evolution. This qualitatively differs from the real-time evolution which usually induces linear growth of entanglement. We also prove analogous bounds for the Rényi entanglement of purification and the entanglement of formation. Our analysis is based on a polynomial approximation to the exponential function which provides a relationship between the imaginary-time evolution and random walks. Moreover, for one-dimensional (1D) systems with $n$ spins, we prove that the Gibbs state is well-approximated by a matrix product operator with a sublinear bond dimension of $e^{\sqrt{\tilde{\mathcal{O}}(β\log(n))}}$. This proof allows us to rigorously establish, for the first time, a quasi-linear time classical algorithm for constructing an MPS representation of 1D quantum Gibbs states at arbitrary temperatures of $β= o(\log(n))$. Our new technical ingredient is a block decomposition of the Gibbs state, that bears resemblance to the decomposition of real-time evolution given by Haah et al., FOCS'18.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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