Summary
Various kinds of condensed matter are mentioned, and bonding types are briefly presented. The most common crystal structures are described. Wave eigenfunctions in periodic media, such as a crystalline solid, are characterized by a phase, \( {\o} = k \cdot r \), and an amplitude of the same periodicity as the underlying medium, according to the so-called Bloch’s theorem; ħk is called crystal momentum and its physical content remains unaffected by the addition of ħG, where G is any vector of the so-called reciprocal lattice. In the latter, Bragg planes and Brillouin zones are defined.
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Further Reading
R. A. L. Jones, Soft condensed matter, [M68].
W. Hamley, Introduction to Soft Matter: Polymer, Colloids, Amphiphiles, and Liquid Crystals, [M69] and [M72].
G. Strobl, The Physics of Polymers, [M70].
P.G. de Gennes, The physics of Liquid Crystals, [M71].
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© 2010 Springer-Verlag Berlin Heidelberg
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Economou, E.N. (2010). A First Acquaintance with Condensed Matter. In: The Physics of Solids. Graduate Texts in Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-02069-8_3
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DOI: https://doi.org/10.1007/978-3-642-02069-8_3
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