5H superHeavy Hydrogen by A.V. BELOZYOROV,


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8b would contribute an impulsive tensile force to its bonds, but a collision between a3 and b in that configuration is less likely because of steric shielding and, as verified in simulations, occurs less frequently. A second simulation focused on the roles of the forces on a generic atom b in a melt caused by nonbonded interactions and those caused by the forces in its connecting bonds, and on the manner in which these forces varied with the reduced density rà of the system: Referring to Fig. 8a, let e1 and e2 be unit vectors directed along the bonds from b to a1 and a2 , respectively.

Sci. Eng. 11, R33-R68. MULTIPLE AMORPHOUS–AMORPHOUS TRANSITIONS THOMAS LOERTING Institute of Physical Chemistry, University of Innsbruck, Innrain 52a, A-6020 Innsbruck, Austria VADIM V. BRAZHKIN Institute for High Pressure Physics, Troitsk, Moscow Region, 142190 Russia TETSUYA MORISHITA Research Institute for Computational Sciences (RICS), National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1 Umezono, Tsukuba, Ibaraki, 305-8568 Japan CONTENTS I. Introduction II.

This leads first to higher transformation pressures as compared with crystalline prototypes and, second to the impossibility of retaining a high coordination number after decompression, which is another fact that strongly differentiates the glasses from their crystalline counterparts. Finally, these high elastic stresses in overconstrained amorphous networks cause a higher tendency to nanocrystallization of such glasses. This is, even to a greater extent, true of oxide glasses with the coordination number Z > 6.

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