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Structure and superconductivity in the binary Re1−xMox alloys

T. Shang, D. J. Gawryluk, J. A. T. Verezhak, E. Pomjakushina, M. Shi, M. Medarde, J. Mesot, T. Shiroka

DOI 10.1103/PhysRevMaterials.3.024801 · Physical Review Materials

T1

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Abstract

The binary Re1−xMox alloys, known to cover the full range of solid solutions, were successfully synthesized and their crystal structures and physical properties investigated via powder x-ray diffraction, electrical resistivity, magnetic susceptibility, and heat capacity. By varying the Re/Mo ratio, we explore the full Re1−xMox binary phase diagram, in all its four different solid phases: hcp-Mg (P63/mmc), α-Mn (I4¯3m), β-CrFe (P42/mnm), and bcc-W (Im3¯m), of which the second is noncentrosymmetric with the rest being centrosymmetric. All Re1−xMox alloys are superconductors, whose critical temperatures exhibit a peculiar phase diagram, characterized by three different superconducting regions. In most alloys, the Tc is almost an order of magnitude higher than in pure Re and Mo. Low-temperature electronic specific-heat data evidence a fully gapped superconducting state, whose enhanced gap magnitude and specific-heat discontinuity suggest a moderately strong electron-phonon coupling across the series. Considering that several α-Mn-type ReT alloys (T = transition metal) show time-reversal symmetry breaking (TRSB) in the superconducting state, while TRS is preserved in the isostructural Mg10Ir19B16 or Nb0.5Os0.5, the Re1−xMox alloys represent another suitable system for studying the interplay of space-inversion, gauge, and time-reversal symmetries in future experiments expected to probe TRSB in the ReT family.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Re0.88Mo0.12

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—Pressure not reportedunknown
Re0.77Mo0.23

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—Pressure not reportedunknown
Re0.6Mo0.4

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—Pressure not reportedunknown
Re0.4Mo0.6

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13Pressure not reportedonset
CePt3Si

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—Pressure not reportedunknown
CeIrSi3

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—Pressure not reportedunknown
Li2Pt3B

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—Pressure not reportedunknown
K2Cr3As3

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—Pressure not reportedunknown
YBiPt

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—Pressure not reportedunknown
LaNiC2

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—Pressure not reportedunknown
Y2C3

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—Pressure not reportedunknown
YPtBi

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—Pressure not reportedunknown
BiPd

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—Pressure not reportedunknown
PbTaSe2

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—Pressure not reportedunknown
Mg10Ir19B16

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—Pressure not reportedunknown
Nb0.5Os0.5

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—Pressure not reportedunknown
Sr2RuO4

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—Pressure not reportedunknown
PrOs4Ge12

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—Pressure not reportedunknown
LaNiGa2

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—Pressure not reportedunknown
Re3W

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—Pressure not reportedunknown

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