Robust superconducting state in the low-quasiparticle-density organic metals β(BEDTTTF)4[(H3O)M(C2O4)3]Y: Superconductivity due to proximity to a charge-ordered state

A. F. Bangura, A. I. Coldea, J. Singleton, A. Ardavan, A. Akutsu-Sato, H. Akutsu, S. S. Turner, P. Day, T. Yamamoto, and K. Yakushi
Phys. Rev. B 72, 014543 – Published 27 July 2005

Abstract

We report magnetotransport measurements on the quasi-two-dimensional charge-transfer salts β(BEDTTTF)4[(H3O)M(C2O4)3]Y, with Y=C6H5NO2 and C6H5CN using magnetic fields of up to 45 T and temperatures down to 0.5 K. A surprisingly robust superconducting state with an in-plane upper critical field Bc233T, comparable to the highest critical field of any BEDT-TTF superconductor, and critical temperature Tc7K is observed when M=Ga and Y=C6H5NO2. The presence of magnetic M ions reduces the in-plane upper critical field to 18T for M=Cr and Y=C6H5NO2 and M=Fe and Y=C6H5CN. Prominent Shubnikov–de Haas oscillations are observed at low temperatures and high magnetic fields, showing that the superconducting salts possess Fermi surfaces with one or two small quasi-two-dimensional pockets, their total area comprising 6% of the room-temperature Brillouin zone; the quasiparticle effective masses were found to be enhanced when the ion M was magnetic (Fe or Cr). The low effective masses and quasiparticle densities, and the systematic variation of the properties of the β(BEDTTTF)4[(H3O)M(C2O4)3]Y salts with unit-cell volume points to the possibility of a superconducting groundstate with a charge-fluctuation-mediated superconductivity mechanism such as that proposed by Merino and McKenzie [Phys. Rev. Lett. 87, 237002 (2001)], rather than the spin-fluctuation mechanism appropriate for the κ(BEDTTTF)2X salts.

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  • Received 7 September 2004

DOI:https://doi.org/10.1103/PhysRevB.72.014543

©2005 American Physical Society

Authors & Affiliations

A. F. Bangura and A. I. Coldea

  • Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom

J. Singleton

  • National High Magnetic Field Laboratory, Los Alamos National Laboratory, TA-35, MS-E536, Los Alamos, New Mexico 87545, USA

A. Ardavan

  • Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom

A. Akutsu-Sato*, H. Akutsu, S. S. Turner, and P. Day

  • Davy-Faraday Research Laboratory, The Royal Institution, 21 Albemarle Street, London, W1X 4BS, United Kingdom

T. Yamamoto and K. Yakushi

  • Institute for Molecular Science, Myodaiji, 444-8585 Okazaki, Japan

  • *Present address: Research Centre for Spectrochemistry, Graduate School of Science, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo, 113-0033, Japan.
  • Present address: Department of Material Science, Graduate School and Faculty of Science, Himeji Institute of Technology, Hyogo 678-1297, Japan.

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Issue

Vol. 72, Iss. 1 — 1 July 2005

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