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Coherent quantum phase slip

机译:相干量子相移

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摘要

A hundred years after the discovery of superconductivity, one fundamental prediction of the theory, coherent quantum phase slip (CQPS), has not been observed. CQPS is a phenomenon exactly dual~1 to the Josephson effect; whereas the latter is a coherent transfer of charges between superconducting leads2'3, the former is a coherent transfer of vortices or fluxes across a superconducting wire. In contrast to previously reported observations4" of incoherent phase slip, CQPS has been only a subject of theoretical study~(9-12). Its experimental demonstration is made difficult by quasipartide dissipation due to gapless excitations in nanowires or in vortex cores. This difficulty might be overcome by using certain strongly disordered superconductors near the superconductor-insulator transition. Here we report direct observation of CQPS in a narrow segment of a superconducting loop made of strongly disordered indium oxide; the effect is made manifest through the superposition of quantum states with different numbers of flux quanta13. As with the Josephson effect, our observation should lead to new applications in superconducting electronics and quantum metrology.%“相干量子相滑移”(CQPS)此前直没有在实rn验中观测到。它是一个与“约瑟夫森效应”正rn好对偶的现象,但后者是电荷在超导接触点之rn间的一种相干转移,而CQPS则是涡流或通量rn在整个一根超导线上的一种相干转移。这篇论rn文报告了对插入在一个环中的根强紊乱的氧rn化铟超导线中的cQPs的直接观测.其效应通rn过具有不同通量的量子态的重叠显示出来。同rn其之前的“约瑟夫森效应”一样,CQPS也可能rn会导致超导电子学和量子计量学中创新应用的rn问世。
机译:在发现超导性一百年之后,尚未观察到该理论的一个基本预测,即相干量子相位滑移(CQPS)。 CQPS是约瑟夫森效应的双重对偶现象。后者是超导导线2'3之间电荷的相干传递,前者是涡流或通量在超导线上的相干传递。与先前报道的不相干相移的观察结果“ 4”相反,CQPS只是理论研究的一个主题(9-12)。由于纳米线或涡旋核中的无间隙激发,拟半粒子耗散使它的实验证明变得困难。可以通过在超导体-绝缘体过渡附近使用某些强无序超导体来克服,这里我们直接观察到由强无序氧化铟制成的超导环的狭窄部分中的CQPS;这种效应通过量子态与与“约瑟夫森效应”一样,我们的观察应会导致超导电子学和量子计量学的新应用。%“相干量子相滑移”(CQPS)直没有在实rn验中观测到。一个与“约瑟夫森效应”正rn好对偶的现象,但另一边是一对在串联在超导接触点之内的一种相干转移,而CQPS则是涡流或通量rn在整个一根超导线上的一种相干转移。这篇论证文报告了对插入在一个环中的根强扭曲乱的氧rn化反相超导线中的cQPs的直接观测。其效应通rn过具有不同通量的量子态的重叠。显示出来。同rn其之前的“约瑟夫森效应”一样,CQPS也可能rn会导致超导电子学和量子计量学中创新应用的rn问世。

著录项

  • 来源
    《Nature》 |2012年第7394期|p.355-358C3|共5页
  • 作者单位

    NEC Green Innovation Research Laboratories, 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501 Japan,The Institute of Physical and Chemical Research (RIKEN), 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501,Japan;

    Center for Materials Theory, Department of Physics and Astronomy, Rutgers University, 136Frelinghuysen Road, Piscataway, New Jersey 08854, USA;

    NEC Green Innovation Research Laboratories, 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501 Japan,The Institute of Physical and Chemical Research (RIKEN), 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501,Japan;

    NEC Green Innovation Research Laboratories, 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501 Japan,The Institute of Physical and Chemical Research (RIKEN), 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501,Japan,Department of Physics, Lancaster University,Lancaster LAI 4YB, UK;

    University of Jyvaskyla, Department of Physics, PB 35,40014 Jyvaskyla, Finland,Moscow State University, Institute of Nuclear Physics, Leninskie gory, GSP-1, Moscow 119899.Russia;

    Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel;

    Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel;

    NEC Green Innovation Research Laboratories, 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501 Japan,The Institute of Physical and Chemical Research (RIKEN), 34 Miyukigaoka,Tsukuba, Ibaraki, 305-8501,Japan;

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