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Titlebook: Quantum Theory of the Solid State; An Introduction Lev Kantorovich Book 2004 Springer Science+Business Media Dordrecht 2004 Potential.X-Ray

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esearchers, drug formulation scientists, drug delivery and drug disposition scientists, as well as clinicians involved in designing and developing novel therapeutics for the back of the eye diseases. This book 978-1-4614-2819-0978-1-4419-9920-7Series ISSN 2210-7371 Series E-ISSN 2210-738X
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Binding in Crystals,ral question that one can ask about any system consisting of more than one atom, e.g. a molecule. Indeed, a solid can be thought of as a very big molecule. Therefore, our analysis will be in great extent based on the . understanding of bonding; after all, today’s knowledge in chemistry is based on q
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Atomic vibrations,g only the first (electronic) equation of the adiabatic approximation (Eq. (3.4), section 3.1) with zero nuclear kinetic energy, i.e. atoms assumed to be .. In this Chapter we will make the next step and consider the second equation of the adiabatic approximation, i.e Eq. (3.12). Thus, we shall take
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Magnetism,mainly concerned with . (induced magnetic moment is directed along the applied magnetic field), . (opposite to the field) and also . and . where spontaneous magnetisation (without any applied field) and other interesting properties are observed. We shall start by recalling several important points f
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Superconductivity, behave as normal. This effect is called . (H. K. Onnes, 1911) and the corresponding metals are .. .. varies widely for different metals (Rh: 0.001 K; Ti: 0.39 K; Al: 1.14 K; V: 5.38 K; Nb: 9.5 K; Nb3Sn: 18.05 K; Nb.Ge: 23.2 K; YBa.Cu.O.: 90 K). At . > .. we talk about . and when . < .. — . states o
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Dielectric materials, ., i.e. the dipole moment . per unit volume takes on some value. As a result, the electric field . inside dielectrics is not equal to zero — quite opposite to what is known to happen in metals. Since dielectrics do not possess a “sea” of free electrons, the electronic density associated with valenc
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Dielectric materials,ributions: (.) the so-called . caused by the distortion of the electron density (e.g. that on atoms and bonds) and (ii) the . due to displacement of atomic nuclei from the lattice sites. The microscopic definition of polarisation has some subtleties in it and we shall start this Chapter by discussing this important point.
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