An unusual phase transition to a second liquid vortex phase in the superconductor YBa2Cu3O7

F. Bouquet (), C. Marcenat, E. Steep, R. Calemczuk, W. K. Kwok, U. Welp, G. W. Crabtree, R. A. Fisher, N. E. Phillips and A. Schilling
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F. Bouquet: Service de Physique, Magnétisme et Supraconductivité, CEA-Grenoble
C. Marcenat: Service de Physique, Magnétisme et Supraconductivité, CEA-Grenoble
E. Steep: Service de Physique, Magnétisme et Supraconductivité, CEA-Grenoble
R. Calemczuk: Service de Physique, Magnétisme et Supraconductivité, CEA-Grenoble
W. K. Kwok: Argonne National Laboratory
U. Welp: Argonne National Laboratory
G. W. Crabtree: Argonne National Laboratory
R. A. Fisher: University of California and Lawrence Berkeley National Laboratory
N. E. Phillips: University of California and Lawrence Berkeley National Laboratory
A. Schilling: Physik-Institut der Universität Zürich

Nature, 2001, vol. 411, issue 6836, 448-451

Abstract: Abstract A magnetic field penetrates a superconductor through an array of ‘vortices’, each of which carries one quantum of flux that is surrounded by a circulating supercurrent. In this vortex state, the resistivity is determined by the dynamical properties of the vortex ‘matter’. For the high-temperature copper oxide superconductors (see ref.1 for a theoretical review), the vortex phase can be a ‘solid’, in which the vortices are pinned, but the solid can ‘melt’ into a ‘liquid’ phase, in which their mobility gives rise to a finite resistance. (This melting phenomenon is also believed to occur in conventional superconductors, but in an experimentally inaccessible part of the phase diagram2.) For the case of YBa2Cu3O7, there are indications of the existence of a critical point, at which the character of the melting changes3,4,5,6,7,8,9,10. But neither the thermodynamic nature of the melting, nor the phase diagram in the vicinity of the critical point, has been well established. Here we report measurements of specific heat and magnetization that determine the phase diagram in this material to 26 T, well above the critical point. Our results reveal the presence of a reversible second-order transition above the critical point. An unusual feature of this transition—namely, that the high-temperature phase is the less symmetric in the sense of the Landau theory11—is in accord with theoretical predictions12,13,14 of a transition to a second vortex-liquid phase.

Date: 2001
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DOI: 10.1038/35078016

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