Observation of Metal–Insulator Transition in Hollandite Vanadate, K<sub>2</sub>V<sub>8</sub>O<sub>16</sub>

  • Isobe Masahiko
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo
  • Koishi Shigenori
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo
  • Kouno Naomi
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo
  • Yamaura Jun-Ichi
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo
  • Yamauchi Touru
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo
  • Ueda Hiroaki
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo
  • Gotou Hirotada
    Division of New Materials Science, Institute for Solid State Physics, University of Tokyo
  • Yagi Takehiko
    Division of New Materials Science, Institute for Solid State Physics, University of Tokyo
  • Ueda Yutaka
    Materials Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo

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  • Observation of Metal–Insulator Transition in Hollandite Vanadate, K2V8O16

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We have synthesized hollandite vanadate, K2V8O16, by a solid-state reaction under 4 GPa at 1473 K for one hour, and investigated its structural and electromagnetic properties. We found a metal–insulator transition with a two-step jump of resistivity of about three orders at around 170 K. The magnetic susceptibility is reduced to a small value at the transition, suggesting the formation of V4+–V4+ singlet pairs and V3+–V3+ pairs in the low-temperature insulator phase. The transition is of first order accompanied by a structural change from a tetragonal to a monoclinic structure. The low-temperature phase has a superlattice of \\sqrt2a×\\sqrt2a×2c, where a and c denote the parameters of the primitive cell for the simple tetragonal hollandite structure, suggesting a charge ordering of V4+ and V3+. We construct a possible charge order model from the obtained results, in which two kinds of double-chain formed by V3+ and V4+ chains and by single V4+ chains order in a manner that gives a superlattice of \\sqrt2×\\sqrt2 in the ab plane. The V4+–V4+ and V3+–V3+ pairs are formed in each chain along the c-axis, resulting in a duplication of the c-axis.

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