Introduction to Solid State Physics |
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Page 302
... equation as a set of linear algebraic equations in the C's . We substitute the Fourier expansion ( 14 ) into the wave equation ( 13 ) . The kinetic energy term is 1 · p2 ( x ) = 2m 1 2m d 12 ( -ih . dx ) 4 ( x ) h2 d24 h2 = = 2m dx2 2m ...
... equation as a set of linear algebraic equations in the C's . We substitute the Fourier expansion ( 14 ) into the wave equation ( 13 ) . The kinetic energy term is 1 · p2 ( x ) = 2m 1 2m d 12 ( -ih . dx ) 4 ( x ) h2 d24 h2 = = 2m dx2 2m ...
Page 303
Charles Kittel. which is a very useful form of the wave equation ( 13 ) . It appears unfamiliar ? only because a set of algebraic equations has emerged in place of the usual dif- ferential equation . The differential equation itself is ...
Charles Kittel. which is a very useful form of the wave equation ( 13 ) . It appears unfamiliar ? only because a set of algebraic equations has emerged in place of the usual dif- ferential equation . The differential equation itself is ...
Page 763
... equations of motion , 728 Landau free energy function , 483 , 486 Landau - Ginzburg equation , 426 Landau theory , Fermi liquid , 256 Landé equation , 504 Langevin - Debye equation , 470 Langevin diamagnetism equation , 500 , 501 ...
... equations of motion , 728 Landau free energy function , 483 , 486 Landau - Ginzburg equation , 426 Landau theory , Fermi liquid , 256 Landé equation , 504 Langevin - Debye equation , 470 Langevin diamagnetism equation , 500 , 501 ...
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