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Critical fields and the spontaneous vortex state in the weakly ferromagnetic superconductor RuSr2GdCu2O8
Journal article   Peer reviewed

Critical fields and the spontaneous vortex state in the weakly ferromagnetic superconductor RuSr2GdCu2O8

C. Y. Yang, B. C. Chang, HUAN-CHIU KU and Y. Y. Hsu
Physical Review B - Condensed Matter and Materials Physics, Vol.72(17), 174508
01/11/2005

Abstract

A spontaneous vortex state (SVS) between 30 and 56 K was observed for the weak-ferromagnetic superconductor RuSr2GdCu2O8 with the ferromagnetic Curie temperature TC=131K and the superconducting transition temperature Tc=56K. The low-field (±20G) super-conducting hysteresis loop indicates a narrow Meissner state region within the average lower critical field Bc1(T)=Bc1(0)[1-(TT0)2], with average Bc1ave(0)=12G and T0=30K. Full Meissner shielding signal in very low applied field indicates an ab plane Bc1ab(0)∼4G with an estimated anisotropic parameter γ∼7 for this layered system. The existence of a spontaneous vortex state between 30 and 56 K is the result of weak-ferromagnetic order with a net spontaneous magnetic moment of ∼0.1μBRu, which generates a weak magnetic dipole field around 10 G in the CuO2 bilayers. The upper critical field Bc2 varies linearly as (1-TTc) up to 7-T field. The vortex melting line Bm varies as (1-TTm)3.5 with melting transition temperature Tm=39K and a very broad vortex liquid region due to the coexistence and the interplay between superconductivity and weak-ferromagnetic order. © 2005 The American Physical Society.

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