TY - JOUR
T1 - Characterization of FeSe single crystals
AU - Takeya, Hiroyuki
AU - Kasahara, Shigeru
AU - Hirata, Kazuto
AU - Mochiku, Takashi
AU - Sato, Akira
AU - Takano, Yoshihiko
PY - 2010/12
Y1 - 2010/12
N2 - Superconductivity at 8 K was reported in β-FeSe with a tetragonal PbO structure but not in δ-FeSe with a hexagonal NiAs structure. The superconducting transition temperature was then increased up to 37 K (on-set) by high pressure on polycrystalline samples. We report a study of the characterization on single crystals of FeSe superconductors. FeSe single crystals were grown using two methods, simple cooling from stoichiometric melt and flux using NaCl/KCl. While a ball-shaped aggregation composed of thick FeSe crystals was grown from the stoichiometric melt, thin hexagonal-shaped crystals with a size up to 1 mm were grown using the NaCl/KCl flux. The two different crystals indicated superconductivity around at 8 K in spite of their hexagonal shape, suggesting a non-superconducting compound with the NiAs-type hexagonal structure. According to the analyses using an X-ray diffractometer and a scanning electron microscope, the crystals contain microcracks that could be caused by stress. We assume that the hexagonal-shaped crystals grown at high temperature may turn partly to tetragonal β-FeSe at the β-δ structure transition temperature.
AB - Superconductivity at 8 K was reported in β-FeSe with a tetragonal PbO structure but not in δ-FeSe with a hexagonal NiAs structure. The superconducting transition temperature was then increased up to 37 K (on-set) by high pressure on polycrystalline samples. We report a study of the characterization on single crystals of FeSe superconductors. FeSe single crystals were grown using two methods, simple cooling from stoichiometric melt and flux using NaCl/KCl. While a ball-shaped aggregation composed of thick FeSe crystals was grown from the stoichiometric melt, thin hexagonal-shaped crystals with a size up to 1 mm were grown using the NaCl/KCl flux. The two different crystals indicated superconductivity around at 8 K in spite of their hexagonal shape, suggesting a non-superconducting compound with the NiAs-type hexagonal structure. According to the analyses using an X-ray diffractometer and a scanning electron microscope, the crystals contain microcracks that could be caused by stress. We assume that the hexagonal-shaped crystals grown at high temperature may turn partly to tetragonal β-FeSe at the β-δ structure transition temperature.
KW - FeSe
KW - Single crystal
KW - Superconductor
KW - X-ray diffraction
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U2 - 10.1016/j.physc.2009.10.041
DO - 10.1016/j.physc.2009.10.041
M3 - Article
AN - SCOPUS:78649698580
SN - 0921-4534
VL - 470
SP - S497-S498
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - SUPPL.1
ER -