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Effects of bonding on superconductivity in Sr(Ni<sub>1−x</sub>Rh<sub>x</sub>)<sub>2</sub>P<sub>2</sub> single crystals

ORAL

Abstract

Bond formation and bond breaking in crystalline intermetallic solids can strongly impact properties associated with delocalized electrons, such as itinerant magnetism and superconductivity. This has been observed on numerous occasions in materials with collapsed tetragonal transitions [1,2,3]. Although SrNi2P2 adopts the common ThCr2Si2 structure for T ≥ 325 K, being in an uncollapsed tetragonal (ucT) state, it is a special case for the ThCr2Si2 class: on cooling below 325 K it adopts a one-third collapsed orthorhombic (tcO) phase where one out of every three P-rows bond across the Sr layers [4,5]. It is also known for exhibiting bulk superconductivity at 1.4 K at ambient pressure [6]. We find that Rh substitution in SrNi2P2 causes a rapid decrease of the one-third collapse transition temperature, as well as an enhancement of superconductivity.

[1] S. Jia et al., Nature Phys. 7, 207 (2011).

[2] U. S. Kaluarachchi et al., Phys. Rev. B 96, 140501(R) (2017).

[3] P. C. Canfield et al., Physica C Supercond. 469, 404 (2009).

[4] V. Keimes et al., Z Anorg Allg Chem 623, 1699 (1997).

[5] J. Schmidt et al., Phys. Rev. B 108, 174415 (2023).

[6] F. Ronning et al., Phys. Rev. B 79, 134507 (2009).

Presenters

  • Juan Schmidt

    Ames National Laboratory, Ames National Laboratory, and Department of Physics and Astronomy, Iowa State University

Authors

  • Juan Schmidt

    Ames National Laboratory, Ames National Laboratory, and Department of Physics and Astronomy, Iowa State University

  • Aashish Sapkota

    Ames National Laboratory

  • Carsyn L Mueller

    Iowa State University

  • Tyler J Slade

    Ames National Laboratory

  • Raquel A. Ribeiro

    Iowa State University

  • Sergey L Bud'ko

    Iowa State University, Ames National Laboratory, and Department of Physics and Astronomy, Iowa State University, Ames National Laboratory and Iowa State University

  • Paul C Canfield

    Iowa State University, Ames National Laboratory, and Department of Physics and Astronomy, Iowa State University, Ames National Laboratory and Iowa State University