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Updated: Jun 9, 2025
Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers
Published on: October 5, 2013
Structural and Superconducting Properties of Bi2Rh3(Se1-S)2 (x = 0-1.0)
Zhiyan Zhang1, Wanli Pan1, Masaki Utsumi1
1Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan.
Abstract:
The structural and superconducting properties of the Bi-based superconductor Bi2Rh3(Se1-S)2 were investigated over a wide pressure range. Bi2Rh3Se2 is a superconductor with a superconducting transition temperature, Tc, of less than ∼1.0 K, whereas Bi2Rh3S2 is a nonsuperconductor. The former shows a clear charge density wave (CDW) phase transition at 240 K and the latter shows a first-order structural phase transition at 165 K, providing the supercell structure. Both compounds have the same crystal structure at ambient temperature and pressure (monoclinic, space group of C2/m (No. 12)). This implies the possible formation of solid solution-like phases Bi2Rh3(Se1-S)2. In this study, we prepared Bi2Rh3(Se1-S)2 (x = 0-1.0) and investigated its superconducting properties and phase transitions at different x values. Because the superconducting properties and temperature causing the phase transition (Tpt) are quite different between Bi2Rh3Se2 and Bi2Rh3S2, their variation against x is quite intriguing from the viewpoint of the pursuit of physical properties via the replacement of Se with S. In this study, the features of the superconductivity and crystal structure against x were fully explored to depict the phase diagram. Moreover, we investigated the pressure (p) dependence of superconductivity and phase transition (CDW or the first-order structural transition) to clarify the interplay between the two ordered states.
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