Supravodivos
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Positive curvature of the thermodynamic transition line in the isotropic superconductor (K,Ba)BiO3 The H-T phase diagram of high-Tc
oxides has been the focus of intense theoretical and experimental works
during the past decade. One of the most striking phenomenon which has been
observed is the existence of a melting line Tm(H)
above which the vortex lattice melts into a liquid of entangled lines.This
melting has very fundamental consequences on the physics of vortices as
the free motion of the flux lines in the liquid state gives rise to a large
dissipation which renders the system useless for applications. Similarly,
the presence of strong thermal fluctuations also renders the determination
of Hc2 difficult from thermodynamic measurements. It
is still unclear whether this upper critical field still exists as a transition
line (or is just some smooth crossover) and what is the "true" (i.e. thermodynamic)
superconducting phase transition line. In order to shed light on this transition,
it was important to perform thermodynamic measurements on a high-Tc
oxide presenting only small thermal fluctuations. We have presented in
[1] specific heat, magneto-tunnelling, reversible magnetization and transport
measurements on high quality (K,Ba)BiO3 single crystals
for which the Ginzburg number Gi is only
~
10-4 (due to its perfectly isotropic structure (i.e. cubic),
a lower Tc ~ 31 K and a coherence
length of the order of 30 Å). Despite those
small thermal fluctuations, we have previously shown that the magneto-transport
data can be well described by the vortex-glass scaling formalism thus suggesting
that the vortex solid melts into a liquid at high temperature through a
second order phase transition. In the following, the vortex-glass transition
field Hvg is defined as the field for which R
0. On the other hand, magnetotunnelling measurements have shown that the
superconducting gap D closes above some characteristic
field
HDand the corresponding HD
(T) line was in reasonable agreement with the classical Werthamer-Helfang-Hohenberg
(WHH) theory for the upper critical field [2]. The physical image emerging
from those measurements was then that of a liquid phase existing for Hvg
< H < HD~ Hc2.
We however show here that the magnetic field HCp is smaller
than HDand presents a strong positive
curvature thus pointing towards a very peculiar nature for the thermodynamic
superconducting transition. This is a totally unexpected feature as in
conventional superconductors the specific heat anomaly enables to define
the upper critical field and thus is expected to vary it linearly with
T close to Tc.
Figure 3: H-Tphase diagram of the (K,Ba)BiO3 system. Squares (HCp(T)): onset on the specific heat anomaly, circles Hvg(T): "vortex-glass transition" line deduced from transport measurements (R 0), triangles: HD(T) defined as the line for which the superconducting gap measures by tunnelling spectroscopy vanishes. [1] S. Blanchard, T. Klein, J. Marcus, I. Joumard, T. Sulpice, P. Szab,
P. Samuely, A.G.M. Jansen, C. Marcenat, Phys. Rev. Lett. 88 (2002), 177201.
P. Szab, P. Samuely S. Blanchard, T. Klein, J. Marcus, I.Joumard (LEPES CNRS Grenoble), C. Marcenat (Commissariat l'Energie Atomique, Grenoble) |