Abstract
Under magnetic fields perpendicular to the conductive plane in quasi-two-dimensional organic conductors: α-(BEDT-TTF)2 MHg(SCN)4 (M= K, Rb, and Tl), the experimentally reported H–T phase diagram has been explained partially. By the self-consistent numerical calculation including the quantum magnetic oscillation and the magnetic breakdown; in addition to the imperfectness of the SDW nesting, we try to completely understand the phase diagram.
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Kishigi, K., Hasegawa, Y. & Miyazaki, M. Magnetic Field–Temperature Phase Diagram of Quasi-Two-Dimensional Organic Conductors Under Magnetic Fields. Journal of Superconductivity 12, 485–488 (1999). https://doi.org/10.1023/A:1007782730574
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DOI: https://doi.org/10.1023/A:1007782730574