By Dr. Siegfried Steeb (auth.)

ISBN-10: 3540043411

ISBN-13: 9783540043416

ISBN-10: 3540359389

ISBN-13: 9783540359388

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Examples are Bi and Ga (Richter and Steeb [256, 305]), in which the amorphous phase at 4~ has the same atomic distribution as the molten state, though dependent from temperature between these two phases a totally different crystalline phase exists. fl) The molten and amorphous phase do not show the same atomic distribution, whereas the amorphous phase has some similarity to the lattice. 8, and for Se finally to 2; 2; 2. According to Glocker [114] in amorphous Ge for example the tetraeder from the lattice is maintained, the similar fact is valid for amorphous As.

In this system there is no additional maximum at increasing concentrations, but there are always two main maxima whose height is shifted continuously. In table 5 tile introduction of a group (Z) and a group of eutectic systems (Eu) was omitted, although in different papers the existence of both phases forming an eutectic mixture in the solid state was evaluated for tile molten state (Bartenev [11, 12, 131, Lashko E194, 197J, Nikonova [220], Hume-Rothery [150], Dutchak E68]) (compare also B 1 2c).

Molten Elements In this section M1 results obtained for molten elements as known from the literature are summarized. It is necessary to establish two groups: On the One hand the metals and on the other hand the semimetals. a) Metals As mentioned in the sections I to I I I of chapter B, the diffraction experiment first of all yields intensity curves. In Fig. 9 as an example for the intensity curves of molten metals the function for molten magnesium [337] as obtained b y the transmission method is given.

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Springer Tracts in Modern Physics, Volume 47 by Dr. Siegfried Steeb (auth.)

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