Abstract
We report and analyze reversible magnetization measurements on a high quality MgB2 single crystal in the vicinity of the zero-field transition temperature, T_{\mathrm {c}}\simeq 38.83 K, at several magnetic fields up to 300 Oe, applied along the c-axis. Although 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 Hi applied along the i-axis cannot grow beyond the limiting magnetic length LHi = (Φ0/(aHi))1/2 with a\simeq 3.12 , 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 a 3D–1D crossover line Hpi(T) = (Φ0/(aξj0−ξk0−))(1−T/Tc)4/3 with i\neq j\neq k and ξi0,j0,k0 ± denotes the critical amplitudes of the correlation lengths above (+) and below (−) Tc along the respective axis. Consequently, above Hpi(T) and T<Tc superconductivity is confined to cylinders with diameter LHi (1D). In contrast, above Tc and Hpi(T) = (Φ0/(aξj0+ξk0+))(T/Tc−1)4/3 the uncondensed pairs are confined to cylinders. Accordingly, there is no continuous phase transition in the (H,T)-plane along the Hc2-lines as predicted by the mean-field treatment.
Weyeneth, S