Based on the creep results, we show that the second magnetization peak coincides with the elastic-to-plastic crossover at low $T$, yet the mechanism changes at higher temperatures. Coexistence of long-range magnetic order and superconductivity: An overview of ternary rare earth compounds. The specimen consists of two phases, each showing threefold symmetry. While Cr1.3Mo6S8 crystallized in a triclinic structure, Mn1.3Mo6S8, Fe1.3Mo6S8, and Ni2.0Mo6S8 crystallized in a hexagonal structure. This article is cited by The solid solutions Mo2Re4S8−xSex (0 ⩽ x ⩽ 8) and Mo2Re4Se8−xTex (0 ⩽ x ⩽ 1.2) are semiconducting, whereas Mo4Re2Te8 is metallic and becomes superconducting at Tc = 3.55 K. motion near the front of magnetization reversal. Zeitschrift f�r anorganische und allgemeine Chemie. Topological Aspects of Chemical Bonding in Superconductors. A molecular-crystal model is proposed for the lattice dynamics of these materials. The two structural forms of Mo15Se19 were found to be superconducting at 4.3K. organic BEDT, Chevrel phase, K3C60, heavy-fermion, and some other superconductors may belong to a unique group of superconductors characterized by large ratios of Tc/TF = 1 10∼ 1 100, which distinguish them from more ordinary BCS superconductors with Tc/TF≤ 1 1000. This material was synthesized at low temperatures by oxidation of In2Mo15Se19 or In3Mo15Se19 by HCl gas. The minor phase corresponds to that described by Guillevic et al. The activation energy barriers Ub(B) extracted from the Arrhenius plots of resistivity are lower for PMS (Ub(9T) = 1570 K) and for SMS (Ub(9T) = 2250 K). The properties of a new superconducting pseudo-one-dimensional compound, Tℓ2Mo6Se6 are presented. However, the corresponding values and temperature dependent Copyright © 2020 Elsevier B.V. or its licensors or contributors. 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