Wednesday, August 22, 2012

1208.4159 (Y. Liu et al.)

Evolution of precipitate morphology during heat treatment and its
implications for the superconductivity in KxFe1.6+ySe2 single crystals
   [PDF]

Y. Liu, Q. Xing, K. W. Dennis, R. W. McCallum, T. A. Lograsso
We study the relationship between precipitate morphology and superconductivity in KxFe1.6+ySe2 single crystals grown by self-flux method. Scanning electron microscopy (SEM) measurements revealed that superconducting phase forms a network in the samples quenched above iron vacancy order-disorder transition temperature Ts. The wavelength of modulated structure varies between 1<{\lambda}<3 \mu m in the micrographs. For the samples obtained by natural cooling down to room temperature in the furnace, referred to as furnace cooling, superconducting phase aggregates into micrometer-sized rectangular bars and aligns as disconnected chains. Accompanying this change in morphology the superconducting shielding fraction is strongly reduced in the furnace-cooling samples. By post-annealing above Ts followed by quenching in room temperature water, the network recovers with superconducting shielding fraction approaching 80%. A reversible change from network to bar chains was realized by a secondary heat treatment in annealed samples showing large shielding fraction, i.e., heating above Ts followed by slow cooling across Ts. The large shielding fraction observed in KxFe1.6+ySe2 single crystals actually results from a uniform and contiguous distribution of superconducting phase. Through the measurements of temperature dependent x-ray diffraction, it is found that the reflection corresponding to superconducting phase merges into that from iron vacancy ordered phase upon warming. It is a solid solution above Ts, where iron atoms randomly occupy the both Fe1 and Fe2 sites in iron vacancy disordering status. By cooling across Ts, superconducting phase precipitates while iron vacancy ordered phase forms together, suggesting that phase separation in KxFe1.6+ySe2 single crystals is driven by the iron vacancy order-disorder transition.
View original: http://arxiv.org/abs/1208.4159

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