Evolution of superconductivity in isovalent Te-substituted K sub(x)Fe sub(2-y)Se sub(2) crystals

We report the evolution of superconductivity and the phase diagram of the K sub(x)Fe sub(2-y)Se sub(2-z)Te sub(z) = 0-0.6) crystals grown by a one-step synthesis. The one-step synthesis is much simpler than a conventional process to grow the K sub(x)Fe sub(2-y)Se sub(2) system. No structural transit...

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Published inSuperconductor science & technology Vol. 26; no. 5; pp. 1 - 5
Main Authors Ozaki, Toshinori, Takeya, Hiroyuki, Deguchi, Keita, Demura, Satoshi, Hara, Hiroshi, Watanabe, Tohru, Denholme, Saleem James, Okazaki, Hiroyuki, Fujioka, Masaya, Yokota, Yoshiko, Yamaguchi, Takahide, Takano, Yoshihiko
Format Journal Article
LanguageEnglish
Published 01.01.2013
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Summary:We report the evolution of superconductivity and the phase diagram of the K sub(x)Fe sub(2-y)Se sub(2-z)Te sub(z) = 0-0.6) crystals grown by a one-step synthesis. The one-step synthesis is much simpler than a conventional process to grow the K sub(x)Fe sub(2-y)Se sub(2) system. No structural transition is observed in any crystals, while lattice parameters exhibit a systematic expansion with increasing Te content. The T sub(c) exhibits a gradual decrease with increasing Te content from T super(onset) sub(c) = 32.9 K at z = 0 to T super(zero) sub(c) = 27.9 K at z = 0.5, followed by a sudden suppression of superconductivity at z = 0.6. Upon approaching a Te concentration of 0.6, the shielding volume fraction decreases and eventually drops to zero. Simultaneously, hump positions in the [rho]-T curve shift to lower temperatures. These results suggest that isovalent substitution of Te for Se in K sub(x)Fe sub(2-y)Se sub(2) crystals suppresses the superconductivity in this system.
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ISSN:0953-2048
1361-6668
DOI:10.1088/0953-2048/26/5/055002