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arXiv 2401.09007quant-phcond-mat.mes-hallmath-phmath.MP
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嵌入酉算子中的任意有界算子的量子奇异值变换

Operator quantum singular value transformation: Spectral mapping, design and topological invariants

The University of Osaka(大阪大学);Ritsumeikan University(立命馆大学);Komatsu University(小松大学)

Chusei Kiumi, Yohei Tanaka, Akito Suzuki

AI总结:

本文将QSVT推广到无限维希尔伯特空间中嵌入酉算子的一般有界算子,揭示多项式变换作用于整个算子而非依赖特定基,为量子信息处理与量子动力学提供新分析工具。

摘要:

本研究将量子奇异值变换(QSVT)推广到可能无限维希尔伯特空间上嵌入酉算子的一般有界算子。通过深入的数学探索,我们对QSVT获得了更精细的算子理论理解,从而得到了一种更简洁的方法。关键发现之一是QSVT中的多项式变换本质上作用于整个算子,而非依赖于特定基的选择。我们期望这项研究能为将这些见解应用于量子信息处理中更广泛的问题铺平道路,并为量子动力学(如量子行走)提供分析工具。

英文摘要:

Quantum singular value transformation (QSVT) provides a unifying framework for quantum algorithms by applying the polynomials of quantum signal processing (QSP) to block-encoded matrices. We connect this framework with spectral analysis, design and topological protection in condensed matter physics. Extending QSVT beyond matrices to possibly infinite-dimensional operators (operator QSVT), we establish the following. First, it transforms every block of the operator by the QSP polynomials; no singular value decomposition is needed. Second, a spectral mapping theorem determines the full spectrum of the QSVT operator, including continuous spectra, from the embedded operator through the QSP polynomial, allowing spectral analysis without translation invariance. Third, the spectral mapping turns QSP into spectral design: the QSP phases can stretch, fold and separate the bands and place the eigenvalues. Finally, the kernel sectors that conventional QSVT usually sets aside carry a topological index, invariant under the choice of QSP phases, local perturbations and gap-preserving deformations, which guarantees topologically protected states. These results unify two quantum walks: Szegedy's walk from quantum algorithms and the split-step walk from condensed matter physics. Their kernel sectors encode the graph's Euler characteristic and the difference of bulk winding numbers, respectively. For the split-step walk, QSP breaks chiral symmetry but not the topological protection, and can move the protected state into a continuous band to form a bound state in the continuum (BIC).

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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