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arXiv 2407.03073quant-phcs.CC

超越自然Grover界限的低能量估计与量子态制备

Beating the natural Grover bound for low-energy estimation and state preparation

Harry Buhrman, Sevag Gharibian, Zeph Landau, François Le Gall, Norbert Schuch, Suguru Tamaki

AI总结:

本文提出针对任意k-体哈密顿量的量子算法,在不假设相互作用局域性的条件下,以低于标准Grover平方根加速的运行时间实现低能量估计和量子态制备,核心思想是证明大量相互作用可在可控误差下忽略。

摘要:

估计多体哈密顿量的基态能量是量子物理许多领域的核心任务。在这项工作中,我们给出了量子算法,对于任意给定的$k$-体哈密顿量$H$,分别计算基态能量的估计值,并制备达到该能量的量子态。具体而言,对于任意$\varepsilon>0$,我们的算法以高概率返回$H$的基态能量在加性误差$\varepsilon M$以内的估计值,或返回具有相应能量的量子态。这里,$M$是所有相互作用项的总强度,通常随系统规模呈广延性增长。我们的方法不对输入哈密顿量相互作用项的几何结构或空间局域性作任何假设,因此甚至可以处理长程或全对全相互作用,例如在量子化学中出现的、基于格点的技术失效的情形。在这一完全一般的设定下,我们的算法运行时间按$2^{cn/2}$缩放,其中$c<1$,从而给出了首个打破无结构搜索中标准平方根Grover加速的低能量估计量子算法。我们方法的核心非常简单,依赖于证明在可控误差下可以忽略其中广延比例的相互作用。这最终意味着,即使是任意的$k$-局域哈密顿量,在其低能量空间中也具有结构,表现为指数维度的低能量子空间。

英文摘要:

Estimating ground state energies of many-body Hamiltonians is a central task in many areas of quantum physics. In this work, we give quantum algorithms which, given any $k$-body Hamiltonian $H$, compute an estimate for the ground state energy and prepare a quantum state achieving said energy, respectively. Specifically, for any $\varepsilon>0$, our algorithms return, with high probability, an estimate of the ground state energy of $H$ within additive error $\varepsilon M$, or a quantum state with the corresponding energy. Here, $M$ is the total strength of all interaction terms, which in general is extensive in the system size. Our approach makes no assumptions about the geometry or spatial locality of interaction terms of the input Hamiltonian and thus handles even long-range or all-to-all interactions, such as in quantum chemistry, where lattice-based techniques break down. In this fully general setting, the runtime of our algorithms scales as $2^{cn/2}$ for $c<1$, yielding the first quantum algorithms for low-energy estimation breaking a standard square root Grover speedup for unstructured search. The core of our approach is remarkably simple, and relies on showing that an extensive fraction of the interactions can be neglected with a controlled error. What this ultimately implies is that even arbitrary $k$-local Hamiltonians have structure in their low energy space, in the form of an exponential-dimensional low energy subspace.

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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