4.8 Article

Observation of superconducting diode effect

Journal

NATURE
Volume 584, Issue 7821, Pages 373-+

Publisher

NATURE RESEARCH
DOI: 10.1038/s41586-020-2590-4

Keywords

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Funding

  1. JSPS KAKENHI [15H05702, 15H05884, 15H05745, 17H04924, 18K19021, 18H04225, 18H01178, 18H05227, 18H01815, 19K21972, 26103002]
  2. Cooperative Research Project Program of the Research Institute of Electrical Communication, Tohoku University
  3. Collaborative Research Program of the Institute for Chemical Research, Kyoto University
  4. Grants-in-Aid for Scientific Research [18H01815, 18K19021, 18H04225, 18H01178, 19K21972, 18H05227] Funding Source: KAKEN

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Nonlinear optical and electrical effects associated with a lack of spatial inversion symmetry allow direction-selective propagation and transport of quantum particles, such as photons(1) and electrons(2-9). The most common example of such nonreciprocal phenomena is a semiconductor diode with a p-n junction, with a low resistance in one direction and a high resistance in the other. Although the diode effect forms the basis of numerous electronic components, such as rectifiers, alternating-direct-current converters and photodetectors, it introduces an inevitable energy loss due to the finite resistance. Therefore, a worthwhile goal is to realize a superconducting diode that has zero resistance in only one direction. Here we demonstrate a magnetically controllable superconducting diode in an artificial superlattice [Nb/V/Ta](n) without a centre of inversion. The nonreciprocal resistance versus current curve at the superconducting-to-normal transition was clearly observed by a direct-current measurement, and the difference of the critical current is considered to be related to the magnetochiral anisotropy caused by breaking of the spatial-inversion and time-reversal symmetries(10-13). Owing to the nonreciprocal critical current, the [Nb/V/Ta](n) superlattice exhibits zero resistance in only one direction. This superconducting diode effect enables phase-coherent and direction-selective charge transport, paving the way for the construction of non-dissipative electronic circuits.

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