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Long-range supercurrents through a chiral non-collinear antiferromagnet in lateral Josephson junctions.


ABSTRACT: The proximity-coupling of a chiral non-collinear antiferromagnet (AFM)1-5 with a singlet superconductor allows spin-unpolarized singlet Cooper pairs to be converted into spin-polarized triplet pairs6-8, thereby enabling non-dissipative, long-range spin correlations9-14. The mechanism of this conversion derives from fictitious magnetic fields that are created by a non-zero Berry phase15 in AFMs with non-collinear atomic-scale spin arrangements1-5. Here we report long-ranged lateral Josephson supercurrents through an epitaxial thin film of the triangular chiral AFM Mn3Ge (refs. 3-5). The Josephson supercurrents in this chiral AFM decay by approximately one to two orders of magnitude slower than would be expected for singlet pair correlations9-14 and their response to an external magnetic field reflects a clear spatial quantum interference. Given the long-range supercurrents present in both single- and mixed-phase Mn3Ge, but absent in a collinear AFM IrMn16, our results pave a way for the topological generation of spin-polarized triplet pairs6-8 via Berry phase engineering15 of the chiral AFMs.

SUBMITTER: Jeon KR 

PROVIDER: S-EPMC8463295 | biostudies-literature | 2021 Oct

REPOSITORIES: biostudies-literature

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Long-range supercurrents through a chiral non-collinear antiferromagnet in lateral Josephson junctions.

Jeon Kun-Rok KR   Hazra Binoy Krishna BK   Cho Kyungjune K   Chakraborty Anirban A   Jeon Jae-Chun JC   Han Hyeon H   Meyerheim Holger L HL   Kontos Takis T   Parkin Stuart S P SSP  

Nature materials 20210805 10


The proximity-coupling of a chiral non-collinear antiferromagnet (AFM)<sup>1-5</sup> with a singlet superconductor allows spin-unpolarized singlet Cooper pairs to be converted into spin-polarized triplet pairs<sup>6-8</sup>, thereby enabling non-dissipative, long-range spin correlations<sup>9-14</sup>. The mechanism of this conversion derives from fictitious magnetic fields that are created by a non-zero Berry phase<sup>15</sup> in AFMs with non-collinear atomic-scale spin arrangements<sup>1-5</  ...[more]

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