By E. A. Brener, M. B. Geilikman, E. D. Temkin (auth.), Kh. S. Bagdasarov, É. L. Lube (eds.)
Papers from the 6th All-Union convention on development of Crystals contain quantity sixteen of this sequence. The articles have been selected which will extra totally elucidate the elemental difficulties of crystal progress as mirrored in family and overseas stories and in unique experiences. This quantity involves six elements. half I is dedicated to mechanisms of crystal progress which are very important for construction of fabrics with given houses. This half examines the temporal evolution of an inhomogeneous kingdom and the array of semicellular and eutectic buildings in the course of microstructure formation, the influence of impurity at the nonequi librium emptiness focus in a turning out to be crystal, and the function of soluble and insoluble impurities within the beginning and progress of crystals. half II bargains with the synthesis and electrophysical houses of novel sturdy electrolytes which are promis ing for functional use, research and correlation of the big quantity of knowledge on progress through the Bridgman-Stockbar ger approach to unmarried crystals of fluorite levels faraway from stoichiometry, and the hydrothermal chemistry and development of hexagonal germanium dioxide.
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Papers from the 6th All-Union convention on progress of Crystals contain quantity sixteen of this sequence. The articles have been selected to be able to extra totally elucidate the fundamental difficulties of crystal development as mirrored in family and overseas studies and in unique reviews. This quantity involves six components.
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Dissolution and division of a dendrite branch between two lycopodium particles in cyclohexanol with added water. Thus, solid particles can be a source of local concentration inhomogeneities of impurity atoms which not only facilitate a premature loss of planar front stability, particle incorporation, and dendrite breakdown, but also seem to cause division of dendrite branches. Exactly such a case is shown in Fig. 5. Here particles in the melt are located at sufficiently close distances and the elevated concentration fields overlap.
4. 5. 6. 7. 8. 9. 29 V. V. Voronkov, I. V. Stepantsova, R. I. Gloriozova, and Yu. N. BoI'sheva, "Impurity capture coefficients in gallium arsenide as functions of concentration," Abstracts of Papers of the VlIth Conf. on Processes of Growth and Synthesis of Semiconducting Crystals and Films [in Russian], Novosibirsk (1986), Vol. 2, pp. 208-209. V. T. Bublik, M. G. MiI'vidskif, and V. B. Osvenskif, "Nature and behavior of point defects in doped single crystals of A3B5 compounds," Izv. JYssh. Uchebn.
Interaction of the particle with the face growing in layers leads to a facial distortion which is completely "healed" after incorporation of the particle. A curved depression which is retained due to isotropic growth even after complete inclusion of the particle into the crystal (Fig. 4) is formed with particle incorporation by a smooth face (normal growth mechanism). Cells, and then dendrites, which undergo morphological changes upon encountering particles, begin to form with increased melt undercooling and a correspondingly increased growth rate.
