2 research outputs found
Magnetic field induced 3D to 1D crossover in Sr0:9La0:1CuO2
The effect of the magnetic field on the critical behavior of Sr0:9La0:1CuO2
is explored in terms of reversible magnetization data. As the correlation
length transverse to the magnetic field Hi,applied along the i-axis, cannot
grow beyond the limiting magnetic length LHi, related to the average distance
between vortex lines, one expects a magnetic field induced finite size effect.
Invoking the scaling theory of critical phenomena we provide clear evidence for
this effect. It implies that in type II superconductors there is a 3D to 1D
crossover line Hpi(T). Consequently, below Tc and above Hpi(T) uperconductivity
is confined to cylinders with diameter LHi(1D). Accordingly, there is no
continuous phase transition in the (H,T)-plane along the Hc2-lines as predicted
by the mean-field treatment.Comment: 4 pages, 5 figure
Probing superconductivity in MgB2 confined to magnetic field tuned cylinders by means of critical fluctuations
We report and analyze reversible magnetization measurements on a high quality
MgB2 single crystal in the vicinity of the zero field transition temperature,
T_c=38.83 K, at several magnetic fields up to 300 Oe, applied along the c-axis.
Though MgB2 is a two gap superconductor our scaling analysis uncovers
remarkable consistency with 3D-xy critical behavior, revealing that close to
criticality the order parameter is a single complex scalar as in 4He. This
opens up the window onto the exploration of the magnetic field induced finite
size effect, whereupon the correlation length transverse to the applied
magnetic field H_i applied along the i-axis cannot grow beyond the limiting
magnetic length L_Hi, related to the average distance between vortex lines. We
find unambiguous evidence for this finite size effect. It implies that in type
II superconductors, such as MgB2, there is the 3D to 1D crossover line H_pi and
xi denotes the critical amplitudes of the correlation lengths above and below
T_c along the respective axis. Consequently, above H_pi(T) and T<T_c
superconductivity is confined to cylinders with diameter L_Hi (1D). In
contrast, above T_c the uncondensed pairs are confined to cylinders.
Accordingly, there is no continuous phase transition in the (H,T)-plane along
the H_c2-lines as predicted by the mean-field treatment