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Spontaneously polarized half-gapped superconductivity

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arxiv 1811.11808 v3 pith:UGL5STQW submitted 2018-11-28 cond-mat.supr-con

classification cond-mat.supr-con
keywords electronssuperconductivitydiscoveryexcitationsferromagneticinformationnonunitaryquantum
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Nonunitary superconductivity is a rare and striking phenomenon in which spin up and spin down electrons segregate into two different quantum condensates. Because they support topological excitations, such superconductors are being seriously considered for potential quantum information applications. We report the discovery of nonunitary spin-triplet superconductivity in UTe2, featuring the high transition temperature of 1.6 K and a remarkably large and anisotropic upper critical field exceeding 40 T. In this unusual superconducting state, electrons with parallel spins pair, yet only half of the available electrons participate, yielding a spin-polarized condensate that coexists with a spin-polarized metal. The superconducting order parameter, which breaks both gauge and time reversal symmetries, arises from strong ferromagnetic fluctuations, placing UTe2 as the paramagnetic end member of the ferromagnetic superconductor series. This discovery yields a new platform for encoding information using topological excitations and for manipulation of spinpolarized currents.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Spin-Orbit Coupling Induced Degeneracy in the Anisotropic Unconventional Superconductor UTe$_2$

    cond-mat.supr-con 2019-08 conditional novelty 6.0 of 10

    DFT+U calculations show that the Fermi level states of UTe2 are dominated by a half-filled, effectively degenerate j=5/2, mj=±1/2 pair, offering a basis for its half-gapped superconducting state.

  2. High-field moment polarization in the itinerant ferromagnet URhSi

    cond-mat.str-el 2019-09 conditional novelty 5.0 of 10

    URhSi shows a broad pseudo-metamagnetic crossover near 30-40 T for fields along b, with a magnetization step and resistivity maximum that resemble behavior in URhGe and UTe2.

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