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arXiv quant-ph/0207172quant-ph
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NMR量子信息处理简介

Introduction to NMR Quantum Information Processing

R. Laflamme, E. Knill, D. G. Cory, E. M. Fortunato, T. Havel, C. Miquel, R. Martinez, C. Negrevergne, G. Ortiz, M. A. Pravia, Y. Sharf, S. Sinha, R. Somma, L. Viola

摘要:

在对核磁共振(NMR)的一般介绍之后,我们给出了实现量子算法的基础。我们描述了量子比特是如何实现和控制的RF脉冲,它们的内部相互作用,和梯度场。NMR的一个特点是内部相互作用(由内部哈密顿量给出)总是打开的。我们讨论如何在称为"重新聚焦“的标准NMR方法的帮助下有效地关闭它们。液态NMR实验在室温下进行,导致极端混合(即,几乎随机)的初始状态。尽管有这种高度的随机性,但研究QIP是可能的,因为弛豫时间(计算中有用信号丢失的时间尺度)足够长。我们解释了这个功能如何导致模拟一个纯(非随机)状态的关键能力,通过使用“伪”状态。我们讨论如何“答案”提供的计算是通过测量,以及如何从QIP的理想,投影测量这种测量不同。然后,我们给出了一些简单的量子算法的实现与一个典型的实验结果。最后,我们讨论了到目前为止,我们从NMR QIP中学到了什么,以及未来NMR QIP实验的前景。

英文摘要:

After a general introduction to nuclear magnetic resonance (NMR), we give the basics of implementing quantum algorithms. We describe how qubits are realized and controlled with RF pulses, their internal interactions, and gradient fields. A peculiarity of NMR is that the internal interactions (given by the internal Hamiltonian) are always on. We discuss how they can be effectively turned off with the help of a standard NMR method called ``refocusing''. Liquid state NMR experiments are done at room temperature, leading to an extremely mixed (that is, nearly random) initial state. Despite this high degree of randomness, it is possible to investigate QIP because the relaxation time (the time scale over which useful signal from a computation is lost) is sufficiently long. We explain how this feature leads to the crucial ability of simulating a pure (non-random) state by using ``pseudopure'' states. We discuss how the ``answer'' provided by a computation is obtained by measurement and how this measurement differs from the ideal, projective measurement of QIP. We then give implementations of some simple quantum algorithms with a typical experimental result. We conclude with a discussion of what we have learned from NMR QIP so far and what the prospects for future NMR QIP experiments are.

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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