Introduction to Solid State Physics |
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Page 264
... Experimental values of L at 0 ° C and at 100 ° C as given in Table 4 are in good agreement with ( 56 ) . On purely classical theory with a Maxwellian distribution of velocities , the result is L = 3 ( kg / e ) 2 , very close to ( 56 ) ...
... Experimental values of L at 0 ° C and at 100 ° C as given in Table 4 are in good agreement with ( 56 ) . On purely classical theory with a Maxwellian distribution of velocities , the result is L = 3 ( kg / e ) 2 , very close to ( 56 ) ...
Page 264
... Experimental values of L at 0 ° C and at 100 ° C as given in Table 4 are in good agreement with ( 56 ) . On purely classical theory with a Maxwellian distribution of velocities , the result is L = 3 ( kg / e ) 2 , very close to ( 56 ) ...
... Experimental values of L at 0 ° C and at 100 ° C as given in Table 4 are in good agreement with ( 56 ) . On purely classical theory with a Maxwellian distribution of velocities , the result is L = 3 ( kg / e ) 2 , very close to ( 56 ) ...
Page 600
... experiments for which the linearity is excellent ; this appears to be largely a matter of the uni- formity of the film . An experimental absorption curve is shown in Fig . 21 . Resonance field in KG 15 14 2200 Å thick 3 600.
... experiments for which the linearity is excellent ; this appears to be largely a matter of the uni- formity of the film . An experimental absorption curve is shown in Fig . 21 . Resonance field in KG 15 14 2200 Å thick 3 600.
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