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Preserving electron spin coherence in solids by optimal dynamical decoupling

机译:通过最佳动力解耦保持固体中的电子自旋相干

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摘要

To exploit the quantum coherence of electron spins in solids in future technologies such as quantum computing, it is first vital to overcome the problem of spin decoherence due to their coupling to the noisy environment. Dynamical decoupling, which uses stroboscopic spin flips to give an average coupling to the environment that is effectively zero, is a particularly promising strategy for combating decoherence because it can be naturally integrated with other desired functionalities, such as quantum gates. Errors are inevitably introduced in each spin flip, so it is desirable to minimize the number of control pulses used to realize dynamical decoupling having a given level of precision. Such optimal dynamical decoupling sequences have recently been explored. The experimental realization of optimal dynamical decoupling in solid-state systems, however, remains elusive. Here we use pulsed electron paramagnetic resonance to demonstrate experimentally optimal dynamical decoupling for preserving electron spin coherence in irradiated malonic acid crystals at temperatures from 50 K to room temperature. Using a seven-pulse optimal dynamical decoupling sequence, we prolonged the spin coherence time to about 30 μs; it would otherwise be about 0.04 μs without control or 6.2 μs under one-pulse control. By comparing experiments with microscopic theories, we have identified the relevant electron spin decoherence mechanisms in the solid. Optimal dynamical decoupling may be applied to other solid-state systems, such as diamonds with nitrogen-vacancy centres, and so lay the foundation for quantum coherence control of spins in solids at room temperature.
机译:为了在诸如量子计算之类的未来技术中利用固体中电子自旋的量子相干性,首先要克服由于自旋相干性与噪声环境耦合而产生的自旋相干性问题。使用频闪自旋翻转使与环境的平均耦合有效地为零的动态去耦是一种非常有希望的解决去相干的策略,因为它可以自然地与其他所需功能集成在一起,例如量子门。在每个自旋翻转中不可避免地会引入误差,因此希望最小化用于实现具有给定精度水平的动态去耦的控制脉冲的数量。最近已经研究了这种最佳的动态解耦序列。然而,在固态系统中实现最佳动态解耦的实验实现仍然难以捉摸。在这里,我们使用脉冲电子顺磁共振来证明在50 K至室温下,在辐照的丙二酸晶体中保持电子自旋相干性的实验性最佳动态解耦。使用七个脉冲的最佳动态去耦序列,我们将自旋相干时间延长到约30μs。否则,在无控制的情况下约为0.04μs,在单脉冲控制下约为6.2μs。通过将实验与微观理论进行比较,我们确定了固体中相关的电子自旋退相干机理。最佳动态解耦可应用于其他固态系统,例如具有氮空位中心的钻石,从而为室温下自旋的量子相干控制奠定了基础。

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  • 来源
    《Nature》 |2009年第7268期|1265-1268|共4页
  • 作者单位

    Hefei National Laboratory for Physical Sciences at Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Hefei National Laboratory for Physical Sciences at Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China;

    Hefei National Laboratory for Physical Sciences at Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Hefei National Laboratory for Physical Sciences at Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, China;

    Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
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  • 正文语种 eng
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  • 入库时间 2022-08-18 02:55:38

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