Introduction to Solid State Physics |
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Page 48
... parallel atomic planes and 2n is the difference in phase between reflections from successive planes . What do we mean by a set of parallel reflecting planes ? Any set of parallel planes will do , provided each plane passes through at ...
... parallel atomic planes and 2n is the difference in phase between reflections from successive planes . What do we mean by a set of parallel reflecting planes ? Any set of parallel planes will do , provided each plane passes through at ...
Page 49
... parallel planes of atoms interfere constructively , as in Fig . 2. We consider elastic scattering , so that the wavelength of the photon or neutron is not changed on reflection . Inelastic scattering ( scattering accompanied by the ...
... parallel planes of atoms interfere constructively , as in Fig . 2. We consider elastic scattering , so that the wavelength of the photon or neutron is not changed on reflection . Inelastic scattering ( scattering accompanied by the ...
Page 519
Charles Kittel. Total energy , kinetic + magnetic , of electrons Parallel to field Opposite to field ( a ) Fermi level Parallel to field - 2μ Β Density of states ( b ) Density of states Figure 12 Pauli paramagnetism at absolute zero ...
Charles Kittel. Total energy , kinetic + magnetic , of electrons Parallel to field Opposite to field ( a ) Fermi level Parallel to field - 2μ Β Density of states ( b ) Density of states Figure 12 Pauli paramagnetism at absolute zero ...
Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
Copyright | |
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absolute zero absorption alkali halide alloy antiferromagnet applied field atoms axis boundary Brillouin zone calculated Chapter charge components conduction band conduction electrons crystal structure cubic density dielectric constant dielectric function diffraction dipole direction dislocation dispersion relation effective mass elastic electric field electron concentration electron gas energy gap equation equilibrium excited exciton experimental F center Fermi surface ferroelectric ferromagnetic Figure free electron frequency function given heat capacity hole impurity interaction ionic lattice constant lattice points low temperatures magnetic field magnetic moment magnon metal modes momentum motion nearest neighbors neutron normal nuclear optical orbital paramagnetic particle phase phonon Phys plane polarization positive potential primitive cell quantum reciprocal lattice vector region resonance result room temperature scattering semiconductor shown in Fig space specimen sphere superconducting theory thermal tion transition unit vacancy valence band velocity wavefunction wavelength wavevector x-ray