Superconducting Phase Induced by a Local Structure Transition in Amorphous Sb_{2}Se_{3} under High Pressure.

Superconductivity and Anderson localization represent two extreme cases of electronic behavior in solids. Surprisingly, these two competing scenarios can occur in the same quantum system, e.g., in an amorphous superconductor. Although the disorder-driven quantum phase transition has attracted much attention, its structural origins remain elusive. Here, we discovered an unambiguous correlation between superconductivity and density in amorphous Sb_{2}Se_{3} at high pressure. Superconductivity first emerges in the high-density amorphous (HDA) phase at about 24 GPa, where the density of glass unexpectedly exceeds its crystalline counterpart, and then shows an enhanced critical temperature when pressure induces crystallization at 51 GPa. Ab initio simulations reveal that the bcc-like local geometry motifs form in the HDA phase, arising from distinct "metavalent bonds." Our results demonstrate that HDA phase is critical for the incipient superconductive behavior.

[1]  Volker L. Deringer,et al.  Origins of structural and electronic transitions in disordered silicon , 2021, Nature.

[2]  M. Wuttig,et al.  Metavalent Bonding in Solids: Characteristic Representatives, Their Properties, and Design Options , 2020, physica status solidi (RRL) – Rapid Research Letters.

[3]  T. Klapwijk,et al.  Quantum breakdown of superconductivity in low-dimensional materials , 2020, Nature Physics.

[4]  M. Wuttig,et al.  Chalcogenides by Design: Functionality through Metavalent Bonding and Confinement , 2020, Advanced materials.

[5]  S. Raoux,et al.  Spin memory of the topological material under strong disorder , 2019, npj Quantum Materials.

[6]  M. Wuttig,et al.  Persistence of spin memory in a crystalline, insulating phase-change material , 2019, npj Quantum Materials.

[7]  M. Wuttig,et al.  Understanding the Structure and Properties of Sesqui‐Chalcogenides (i.e., V2VI3 or Pn2Ch3 (Pn = Pnictogen, Ch = Chalcogen) Compounds) from a Bonding Perspective , 2019, Advanced materials.

[8]  K. T. Law,et al.  Disorder-induced multifractal superconductivity in monolayer niobium dichalcogenides , 2019, Nature Physics.

[9]  Volker L. Deringer,et al.  A Quantum‐Mechanical Map for Bonding and Properties in Solids , 2018, Advanced materials.

[10]  M. Sanquer,et al.  Collective energy gap of preformed Cooper pairs in disordered superconductors , 2018, Nature Physics.

[11]  Matthias Wuttig,et al.  Incipient Metals: Functional Materials with a Unique Bonding Mechanism , 2017, Advanced materials.

[12]  Aiguo Li,et al.  Robust zero resistance in a superconducting high-entropy alloy at pressures up to 190 GPa , 2017, Proceedings of the National Academy of Sciences.

[13]  Wenge Yang,et al.  Ultrastable Amorphous Sb2Se3 Film. , 2017, The journal of physical chemistry. B.

[14]  A. Valladares,et al.  Superconductivity in Bismuth. A New Look at an Old Problem , 2016, PloS one.

[15]  V. Prakapenka,et al.  DIOPTAS: a program for reduction of two-dimensional X-ray diffraction data and data exploration , 2015 .

[16]  H. Mao,et al.  Superconductivity in Strong Spin Orbital Coupling Compound Sb2Se3 , 2014, Scientific Reports.

[17]  R. Ewing,et al.  Sb2Se3 under pressure , 2013, Scientific Reports.

[18]  Wei Zhang,et al.  Role of vacancies in metal-insulator transitions of crystalline phase-change materials. , 2012, Nature materials.

[19]  E. Ma,et al.  Pressure tunes electrical resistivity by four orders of magnitude in amorphous Ge2Sb2Te5 phase-change memory alloy , 2012, Proceedings of the National Academy of Sciences.

[20]  H. Mao,et al.  Peierls distortion mediated reversible phase transition in GeTe under pressure , 2012, Proceedings of the National Academy of Sciences.

[21]  H. Mao,et al.  Pressure-induced reversible amorphization and an amorphous–amorphous transition in Ge2Sb2Te5 phase-change memory material , 2011, Proceedings of the National Academy of Sciences.

[22]  P Jost,et al.  Disorder-induced localization in crystalline phase-change materials. , 2011, Nature materials.

[23]  L. Ioffe,et al.  Localization of preformed Cooper pairs in disordered superconductors , 2010, 1012.3630.

[24]  Y. Avishai,et al.  Nature of the superconductor–insulator transition in disordered superconductors , 2007, Nature.

[25]  S J L Billinge,et al.  PDFfit2 and PDFgui: computer programs for studying nanostructure in crystals , 2007, Journal of physics. Condensed matter : an Institute of Physics journal.

[26]  P. L. Lee,et al.  Polyamorphism in a metallic glass. , 2007, Nature materials.

[27]  Richard Dronskowski,et al.  The role of vacancies and local distortions in the design of new phase-change materials. , 2007, Nature materials.

[28]  P. McMillan,et al.  A density-driven phase transition between semiconducting and metallic polyamorphs of silicon , 2005, Nature materials.

[29]  P. McMillan,et al.  Pressure-induced amorphization and an amorphous–amorphous transition in densified porous silicon , 2001, Nature.

[30]  Andreas Savin,et al.  ELF: The Electron Localization Function , 1997 .

[31]  A. Savin,et al.  Classification of chemical bonds based on topological analysis of electron localization functions , 1994, Nature.

[32]  S. R. Elliott,et al.  Medium-range structural order in covalent amorphous solids , 1991, Nature.

[33]  G. Bergmann Amorphous metals and their superconductivity , 1976 .

[34]  J. Mooij Electrical Conduction in Concentrated Disordered Transition Metal Alloys , 1973, June 16.

[35]  Philip W. Anderson,et al.  Theory of dirty superconductors , 1959 .