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Titlebook: Electrons and Phonons in Layered Crystal Structures; T. J. Wieting,M. Schlüter Book 1979 D. Reidel Publishing Company, Dordrecht, Holland

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书目名称Electrons and Phonons in Layered Crystal Structures
编辑T. J. Wieting,M. Schlüter
视频video
丛书名称Physics and Chemistry of Materials with A
图书封面Titlebook: Electrons and Phonons in Layered Crystal Structures;  T. J. Wieting,M. Schlüter Book 1979 D. Reidel Publishing Company, Dordrecht, Holland
描述This volume is devoted to the electron and phonon energy states of inorganic layered crystals. The distinctive feature of these low-dimensional materials is their easy mechanical cleavage along planes parallel to the layers. This feature implies that the chemical binding within each layer is much stronger than the binding between layers and that some, but not necessarily all, physical properties of layered crystals have two-dimensional character. In Wyckoff‘s Crystal Structures, SiC and related com­ pounds are regarded as layered structures, because their atomic layers are alternately stacked according to the requirements of cubic and hexagonal close-packing. How­ ever, the uniform (tetrahedral) coordination of the atoms in these compounds excludes the kind of structural anisotropy that is fundamental to the materials dis­ cussed in this volume. An individual layer of a layered crystal may be composed of either a single sheet of atoms, as in graphite, or a set of up to five atomic sheets, as in Bi2 Te3‘ A layer may also have more complicated arrangements of the atoms, as we find for example in Sb S . But the unique feature common to all these materials is 2 3 the structural anisotr
出版日期Book 1979
关键词Absorption; Atom; Pseudopotential; Sorption; bonding; crystal structure; metals; structure
版次1
doihttps://doi.org/10.1007/978-94-009-9370-9
isbn_softcover978-94-009-9372-3
isbn_ebook978-94-009-9370-9
copyrightD. Reidel Publishing Company, Dordrecht, Holland 1979
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Electrons and Phonons in Layered Crystal Structures
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Electrons and Phonons in Layered Crystal Structures978-94-009-9370-9
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Book 1979ay be composed of either a single sheet of atoms, as in graphite, or a set of up to five atomic sheets, as in Bi2 Te3‘ A layer may also have more complicated arrangements of the atoms, as we find for example in Sb S . But the unique feature common to all these materials is 2 3 the structural anisotr
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Gerhard Preyer,Maria Ulkan,Alexander Ulfigin the intercalated phases [2]. According to the discussions in Chapter A.3 and similar to non-transition metal compounds the materials can be grouped into . major classes depending on the crystal field symmetry around the metallic ions. The two types of structures, the octahedral and the trigonal p
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nal materials is their easy mechanical cleavage along planes parallel to the layers. This feature implies that the chemical binding within each layer is much stronger than the binding between layers and that some, but not necessarily all, physical properties of layered crystals have two-dimensional
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Hartmann Tyrell,Raf VanderstraetenThe methods will be discussed in the chronological order of appearance of layer compound calculations in the literature. Moreover, this list of methods of band calculations is by no means complete; only common methods as they have been applied to layer compounds are described in detail.
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