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arXiv 1908.03759quant-ph
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用于开放系统动力学和热化模拟的硬件高效量子算法

Hardware-efficient quantum algorithm for the simulation of open-system dynamics and thermalisation

Hong-Yi Su, Ying Li

摘要:

量子开放系统模拟是量子模拟的一个重要范畴。通过模拟零温度下的热化过程,我们可以解决量子系统的基态问题。为了在量子计算机上实现开放系统进化,我们需要使用量子比特对环境进行编码。然而,通常环境比系统大得多,即如果环境被直接编码,则需要许多量子比特。在本文中,我们提出了一种方法来模拟开放系统动态再现水库关联函数使用最小化希尔伯特空间。通过这种方式,我们只需要少量的量子比特来表示环境。为了通过再现高达$n$ -时间关联函数来模拟无时间卷积主方程的$n$-阶展开,表示环境的量子比特的数量是$\sim \lfloor \frac{n}{2} \rfloor \log_2(N_ωN_β)$。这里,$N_ω$是离散化的环境频谱中的频率的数量,并且$N_β$是系统-环境相互作用中的项的数量。通过再生两次关联函数,即取$n = 2$,我们可以模拟马尔可夫量子主方程。在我们的算法中,量子计算机上的环境甚至可以比系统更小。

英文摘要:

The quantum open-system simulation is an important category of quantum simulation. By simulating the thermalisation process at the zero temperature, we can solve the ground-state problem of quantum systems. To realise the open-system evolution on the quantum computer, we need to encode the environment using qubits. However, usually the environment is much larger than the system, i.e. numerous qubits are required if the environment is directly encoded. In this paper, we propose a way to simulate open-system dynamics by reproducing reservoir correlation functions using a minimised Hilbert space. In this way, we only need a small number of qubits to represent the environment. To simulate the $n$-th-order expansion of the time-convolutionless master equation by reproducing up to $n$-time correlation functions, the number of qubits representing the environment is $\sim \lfloor \frac{n}{2} \rfloor \log_2(N_ωN_β)$. Here, $N_ω$ is the number of frequencies in the discretised environment spectrum, and $N_β$ is the number of terms in the system-environment interaction. By reproducing two-time correlation functions, i.e. taking $n = 2$, we can simulate the Markovian quantum master equation. In our algorithm, the environment on the quantum computer could be even smaller than the system.

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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