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Titlebook: Electronic Structure and Properties of Hydrogen in Metals; P. Jena,C. B. Satterthwaite Book 1983 Springer Science+Business Media New York

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https://doi.org/10.1007/978-3-8349-3492-5f preparation. Samples loaded to a concentration of x > 0.6, by avoiding the mixed phase region, have a lattice parameter slightly lower than samples loaded to the same concentration by passing through the mixed phase region. The difference is thought to result from unrelieved strain produced as a r
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https://doi.org/10.1007/978-3-642-00631-9ng the lattice distortions have been determined: The defect volume, the long-range displacement field described by the force dipole tensor, the local displacements of the hydrogen neighbors and the Kanzaki forces necessary to create the observed lattice distortions..Lattice distoritions are closely
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R. Cowan,N. Jonard,J. -B. Zimmermannation has been investigated, whose strength depends on T according to a Curie-Weiss type of relationship. This relaxation effect only partly accounts for the softening of the elastic constants C’ and C induced by hydrogen or deuterium. The moduli are also affected by a positive electronic contributi
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Identifying Ideas and Opportunities, temperature, isotope, and defect concentration. In addition to the stable 2.4 K relaxation peak found earlier by Poker, et. al., an additional peak at 6.3 K at 10 MHz was found when the specimen was rapidly cooled to He temperature. The peak correlated with the resistivity recovery found by Hanada
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Arbeit ohne Zukunft? Zukunft ohne Arbeit?s, e.g., binary alloys, glasses and liquids. The unique features of spinodals in M-H systems are discussed from the point of view of the special nature of the density fluctuations, in the critical point region, for coherent M-H systems. Methods of locating spinodals and detecting spinodal decomposition are reviewed for M-H systems.
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Elena Queck,Kilian Cedl,Steffen Kutteren (M-H) systems. It is observed that the general behavior of the relative partial molar enthalpy of hydrogen, ΔH., is that ΔH. vs x (where x = H/M) tends to exhibit a minimum. This is accounted for by the model as due to the generality of the existence of a repulsive MH interaction and an anti-bonding HH interaction.
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https://doi.org/10.1007/978-3-658-02931-9s generated interest within the theoretical physics community because it is a very close physical realization of the theoretical lattice-gas model. On the other hand, it is also studied as a model substance by those interested in the practical aspects of hydrogen storage and other applications of metal-hydrogen systems.
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Enthalpy of Metal-Hydrogen Systems: A Pair-Bond Modelen (M-H) systems. It is observed that the general behavior of the relative partial molar enthalpy of hydrogen, ΔH., is that ΔH. vs x (where x = H/M) tends to exhibit a minimum. This is accounted for by the model as due to the generality of the existence of a repulsive MH interaction and an anti-bonding HH interaction.
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