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Long-range supercurrents through a chiral non-collinear antiferromagnet in lateral Josephson junctions
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 pairs 6 – 8 , thereby enabling non-dissipative, long-range spin correlations 9 – 14 . The mechanism of t...
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Published in: | Nature materials 2021-10, Vol.20 (10), p.1358-1363 |
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Main Authors: | , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | 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 pairs
6
–
8
, thereby enabling non-dissipative, long-range spin correlations
9
–
14
. The mechanism of this conversion derives from fictitious magnetic fields that are created by a non-zero Berry phase
15
in AFMs with non-collinear atomic-scale spin arrangements
1
–
5
. Here we report long-ranged lateral Josephson supercurrents through an epitaxial thin film of the triangular chiral AFM Mn
3
Ge (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 correlations
9
–
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 Mn
3
Ge, but absent in a collinear AFM IrMn
16
, our results pave a way for the topological generation of spin-polarized triplet pairs
6
–
8
via Berry phase engineering
15
of the chiral AFMs.
Long-range lateral Josephson supercurrents are observed in a chiral non-collinear antiferromagnet, indicating topologically generated triplet pairing states. |
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ISSN: | 1476-1122 1476-4660 |
DOI: | 10.1038/s41563-021-01061-9 |