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Titlebook: Charge Density Waves in Solids; Proceedings of the I Gyula Hutiray,Jenö Sólyom Conference proceedings 1985 Springer-Verlag Berlin Heidelber

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Angebotsspektrum genauer verstehenus-Clapeyron equation. The discrepancy between estimated and measured volume changes at the transition between the NC-phase and the commensurate (C-) phase on cooling is explained by considering the time-dependence of this transition under pressure.
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Neutron and x-ray scattering study on K0.3MoO3 and other quasi one dimensional conductors,scattering techniques in order to see the natures of the electron phonon interaction in materials near the metal-insulator boundary. The transition in K.MoO. may be understood by a band picture. The behavior of the transition in (NbSe.).I cannot be considered simply as the one of the band electrons.
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X-ray study of charge-density wave in K0.30Mo03 under electric fields,W wave vector above the threshold electric field E.. The change occurs mainly in the (2a. - c.) direction which is perpendicular to the one-dimensional axis (b - axis). That also depends on the direction of the electric field and its magnitude. The time resolved X-ray diffraction study showed that t
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Structural and electrical properties interpretation through band structure calculations on the (MSeudo-1D compounds with exciting properties. In these compounds infinite (MX.) chains are well separated from each other by halogen chains. Metal ions are sandwiched by two rectangular chalcogen units with a dihedral angle of approximately 45°. According to n, different sequences of metal-metal distan
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Neutron studies of the blue bronzes K0.3MoO3 and Rb0.3MoO3,ic neutron scattering measurements on these compounds. Some low lying phonon dispersion branches have been measured in the metallic phase. The behaviour of the Kohn anomaly has been studied between room temperature and T.. Below T. the value of the CDW wavevector has been determined as a function of
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The effect of a magnetic field on the discotm1ensurate to commensurate transition in 2H TaSe2, affected by an applied magnetic field. The proposed phase diagram resembles that found as a function of pressure (0–4 GPa) but with magnetic field in the region 0-2 Tesla as the variable..The onset(T. ∼ 123K), lock-in (T.=88K), stripe (T.=92K), and reversion (T.=113K) transitions were monitored by
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