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Chiral singlet superconductivity in the weakly correlated metal LaPt3P.


ABSTRACT: Chiral superconductors are novel topological materials with finite angular momentum Cooper pairs circulating around a unique chiral axis, thereby spontaneously breaking time-reversal symmetry. They are rather scarce and usually feature triplet pairing: a canonical example is the chiral p-wave state realized in the A-phase of superfluid He3. Chiral triplet superconductors are, however, topologically fragile with the corresponding gapless boundary modes only weakly protected against symmetry-preserving perturbations in contrast to their singlet counterparts. Using muon spin relaxation measurements, here we report that the weakly correlated pnictide compound LaPt3P has the two key features of a chiral superconductor: spontaneous magnetic fields inside the superconducting state indicating broken time-reversal symmetry and low temperature linear behaviour in the superfluid density indicating line nodes in the order parameter. Using symmetry analysis, first principles band structure calculation and mean-field theory, we unambiguously establish that the superconducting ground state of LaPt3P is a chiral d-wave singlet.

SUBMITTER: Biswas PK 

PROVIDER: S-EPMC8097077 | biostudies-literature | 2021 May

REPOSITORIES: biostudies-literature

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Chiral singlet superconductivity in the weakly correlated metal LaPt<sub>3</sub>P.

Biswas P K PK   Ghosh S K SK   Zhao J Z JZ   Mayoh D A DA   Zhigadlo N D ND   Xu Xiaofeng X   Baines C C   Hillier A D AD   Balakrishnan G G   Lees M R MR  

Nature communications 20210504 1


Chiral superconductors are novel topological materials with finite angular momentum Cooper pairs circulating around a unique chiral axis, thereby spontaneously breaking time-reversal symmetry. They are rather scarce and usually feature triplet pairing: a canonical example is the chiral p-wave state realized in the A-phase of superfluid He<sup>3</sup>. Chiral triplet superconductors are, however, topologically fragile with the corresponding gapless boundary modes only weakly protected against sym  ...[more]

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