Introduction to Solid State PhysicsNew edition of the most widely-used textbook on solid state physics in the world. Describes how the excitations and imperfections of actual solids can be understood with simple models that have firmly established scope and power. The foundation of this book is based on experiment, application and theory. Several significant advances in the field have been added including high temperature superconductors, quasicrystals, nanostructures, superlattices, Bloch/Wannier levels, Zener tunneling, light-emitting diodes and new magnetic materials. |
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Page 386
... field at a site with a cubic arrangement of neighbors in a crystal of spherical shape . The macroscopic electric field in a sphere is ( CGS ) ( SI ) by ( 10 ) . E = Eo + E1 = Eo - E = Eo + E1 = Eo -- 4π 3 1 3E0 Ꮲ ; P " ( 12 ) But consider ...
... field at a site with a cubic arrangement of neighbors in a crystal of spherical shape . The macroscopic electric field in a sphere is ( CGS ) ( SI ) by ( 10 ) . E = Eo + E1 = Eo - E = Eo + E1 = Eo -- 4π 3 1 3E0 Ꮲ ; P " ( 12 ) But consider ...
Page 410
... electric field averaged over the volume of the specimen defines the macroscopic electric field E of the Maxwell equations . • The electric field that acts at the site r , of an atom j is the local electric field , Eloc . It is a sum ...
... electric field averaged over the volume of the specimen defines the macroscopic electric field E of the Maxwell equations . • The electric field that acts at the site r , of an atom j is the local electric field , Eloc . It is a sum ...
Page 411
... electric field as p = αEloc • The dielectric susceptibility x and dielectric constant e are defined in terms of the macroscopic electric field E as D = E + 4πP = € E = ( 1 + 4πу ) E , or x = P / E . In SI , we have x = P / EOE . • At ...
... electric field as p = αEloc • The dielectric susceptibility x and dielectric constant e are defined in terms of the macroscopic electric field E as D = E + 4πP = € E = ( 1 + 4πу ) E , or x = P / E . In SI , we have x = P / EOE . • At ...
Contents
PERIODIC ARRAYS OF ATOMS | 3 |
1 | 10 |
INDEX SYSTEM FOR CRYSTAL PLANES | 12 |
Copyright | |
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a₁ absolute zero alloys approximation atoms axis band edge Bloch Brillouin zone Chapter charge collision components conduction band conduction electrons crystal structure defined density dielectric diffraction dimensions direction dislocation dispersion relation displacement effective mass elastic electric field electron concentration electron gas energy gap equation equilibrium exciton factor Fermi level Fermi surface ferromagnetic Figure flux Fourier free electron frequency function germanium heat capacity hole impurity integral interaction ionic ions lattice constant lattice point layer low temperatures magnetic field magnetic moment metals modes momentum motion nearest-neighbor neutron normal optical orbital oscillator particle phase phonon plane polarization potential energy primitive cell quantum reciprocal lattice vector resonance result scattering semiconductor shown in Fig silicon solution space specimen sphere spin superconducting Table theory thermal tion transition unit valence band values velocity voltage volume wave wavefunction wavelength wavevector x-ray zone boundary