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Extra resources for Course of Theoretical Physics, Volume 8, Volume 8,: Electrodynamics of Continuous Media
C. 10. 0 J! 5. 5. 2. 11. 62]. 62]. 10. 11 occur only for the small intracluster (Rh,Ru)(Rh,Ru) distances. 62]. 12. 13. Superconducting transition tem- .. 43-45] have shown that the electronic states at the Fermi level in the CeCo 4B4-type MRh4B4 compounds do contain a significant contribution deriving from the boron atoms, consistent with this suggestion. 65]. The Tc data were analyzed as outlined in the last section. 12 is a plot of Tc versus the deGennes factor (dGF). 5, a good fit of the AG theory to the data was obtained for RE = Ho to Lu (solid curve in Fig.
These materials might, therefore, be expected to exhibit physical properties typical of sp-element superconductors. 105,10B, 112,113,117]. 11B]. The lattice parameters of phases I, II and III are simply related: IZ a I ~ alII ~ all ~ cII /2; it is therefore likely that the phase II and phase III structures, not yet reported in detail, have similar features which in turn are similar to those of phase I. 13. 105,108,112,113,117-120]. Re-entrant superconductivity occurs in the phase II compound ErRh 1.
4. 46] suggested a similar value of Tco for the nonmagnetic hypothetical compound LaRh 4B4 . 49], the exchange coupling does not appear to be any stronger in this compound than in the heavy RERh4B4 members. 1b). 36,41,51-53]. 50,51]. 7. The factors contributing to these incipient instabilities are not yet understood, but these may also be important to the superconducting and magnetic interactions in the MRh4B4 compounds at zero pressure. 54]. b) Body-Gentered-TetragonaZ LuRu 4B4 Structure Two high temperature or metastable modifications of the CeC0 4B4-type MRh4B4 compounds have been found to exist.