并行量子计算仿真

B. Cour, S. Lanham, Corey I. Ostrove
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引用次数: 5

摘要

量子计算机提供了一种全新的计算范式,有望彻底改变我们解决广泛问题的能力。令人惊讶的是,基于门的量子计算的基本数学结构,如有限维希尔伯特空间上的幺正运算,并不是量子系统所独有的,而是可以在某些经典系统中找到的。以前,已经证明可以使用嵌套正交调幅信号在经典模拟信号方面表示任意多量子位量子态。此外,使用数字控制的模拟电子学可以操纵这些信号以执行量子门操作并因此执行量子算法。然而,单个信号的计算能力受到所需带宽的限制,当使用基于频率的编码表示时,带宽随量子位的数量呈指数级增长。为了克服这一限制,我们引入了一种方法,将这种方法扩展到多个并行信号。这样做可以用处理频率编码信号所需的相同门时间来模拟更大的量子态。在提出的表示中,信号数量的每增加一倍对应于空间域中的一个额外量子位。单退出门操作被类似地扩展,以便在使用基于频率或空间编码方案表示的量子位上操作。此外,我们描述了一种在使用频率或空间编码表示的量子比特对之间或基于频率和空间编码的量子比特之间执行门操作的方法。最后,我们描述了如何将这种方法扩展到在时域中表示量子位。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Parallel Quantum Computing Emulation
Quantum computers provide a fundamentally new computing paradigm that promises to revolutionize our ability to solve broad classes of problems. Surprisingly, the basic mathematical structures of gate-based quantum computing, such as unitary operations on a finite-dimensional Hilbert space, are not unique to quantum systems but may be found in certain classical systems as well. Previously, it has been shown that one can represent an arbitrary multi-qubit quantum state in terms of classical analog signals using nested quadrature amplitude modulated signals. Furthermore, using digitally controlled analog electronics one may manipulate these signals to perform quantum gate operations and thereby execute quantum algorithms. The computational capacity of a single signal is, however, limited by the required bandwidth, which scales exponentially with the number of qubits when represented using frequency-based encoding. To overcome this limitation, we introduce a method to extend this approach to multiple parallel signals. Doing so allows a larger quantum state to be emulated with the same gate time required for processing frequency-encoded signals. In the proposed representation, each doubling of the number of signals corresponds to an additional qubit in the spatial domain. Single quit gate operations are similarly extended so as to operate on qubits represented using either frequency-based or spatial encoding schemes. Furthermore, we describe a method to perform gate operations between pairs of qubits represented using frequency or spatial encoding or between frequency-based and spatially encoded qubits. Finally, we describe how this approach may be extended to represent qubits in the time domain as well.
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