Introduction to Solid State Physics |
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Page 224
... particle , then in moving from a region at local temperature T + AT to a region at local temperature T a particle will give up energy c AT . Now AT between the ends of a free path of the particle is given by dT dT AT = l = dx dx where 7 ...
... particle , then in moving from a region at local temperature T + AT to a region at local temperature T a particle will give up energy c AT . Now AT between the ends of a free path of the particle is given by dT dT AT = l = dx dx where 7 ...
Page 256
... particle excitations of the system of interacting electrons . These single particle excitations are called quasiparticles ; they have a one - to - one corres- pondence with the single particle excitations of the free electron gas . A ...
... particle excitations of the system of interacting electrons . These single particle excitations are called quasiparticles ; they have a one - to - one corres- pondence with the single particle excitations of the free electron gas . A ...
Page 688
... particle can be traversed by the dislocation , or the particle cannot be traversed by the dislocation . If the particle cannot be cut10 the stress necessary to force a dislocation between particles spaced L apart on a slip plane should ...
... particle can be traversed by the dislocation , or the particle cannot be traversed by the dislocation . If the particle cannot be cut10 the stress necessary to force a dislocation between particles spaced L apart on a slip plane should ...
Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
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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