corner
corner

Phys. Rev. Lett. 99, 187002 (2007) [4 pages]

Calorimetric Evidence for a Fulde-Ferrell-Larkin-Ovchinnikov Superconducting State in the Layered Organic Superconductor κ-(BEDT-TTF)2Cu(NCS)2

Download: PDF (356 kB) Buy this article Export: BibTeX or EndNote (RIS)

R. Lortz1, Y. Wang2, A. Demuer2, P. H. M. Böttger3, B. Bergk3, G. Zwicknagl4, Y. Nakazawa5, and J. Wosnitza3
1Department of Condensed Matter Physics, University of Geneva, CH-1211 Geneva 4, Switzerland
2Grenoble High Magnetic Field Laboratory, CNRS, 38042 Grenoble Cedex 9, France
3Hochfeld-Magnetlabor Dresden (HLD), Forschungszentrum Dresden-Rossendorf, D-01314 Dresden, Germany
4Institut für Mathematische Physik, Technische Universität Braunschweig, D-38106 Braunschweig, Germany
5Department of Chemistry, Osaka University, 1-1, Machikaneyama, Toyonaka, Osaka, Japan

Received 25 June 2007; published 30 October 2007

The specific heat of the layered organic superconductor κ-(BEDT-TTF)2Cu(NCS)2, where BEDT-TTF is bisethylenedithio-tetrathiafulvalene, has been studied in magnetic fields up to 28 T applied perpendicular and parallel to the superconducting layers. In parallel fields above 21 T, the superconducting transition becomes first order, which signals that the Pauli-limiting field is reached. Instead of saturating at this field value, the upper-critical-field increases sharply and a second first-order transition line appears within the superconducting phase. Our results give strong evidence that the phase, which separates the homogeneous superconducting state from the normal state is a realization of a Fulde-Ferrell-Larkin-Ovchinnikov state.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.99.187002
DOI:
10.1103/PhysRevLett.99.187002
PACS:
74.70.Kn, 65.40.Ba, 74.25.Bt, 75.40.Cx