Introduction to Solid State Physics |
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Page 69
... diffraction condition 2k G + G2 = 0 ) First it is convenient to substitute -G for G to obtain the diffraction condition in the form • 2k . GG2 . ( 41 ) The indicated replacement does not change the meaning of the diffraction con- dition ...
... diffraction condition 2k G + G2 = 0 ) First it is convenient to substitute -G for G to obtain the diffraction condition in the form • 2k . GG2 . ( 41 ) The indicated replacement does not change the meaning of the diffraction con- dition ...
Page 93
... diffraction pattern of Fig . 37b ; the axis of the cylinder is coincident with the axis of the linear structure or fiber . Describe the appearance of the diffraction pattern on the film . ( b ) A flat photographic plate is placed behind ...
... diffraction pattern of Fig . 37b ; the axis of the cylinder is coincident with the axis of the linear structure or fiber . Describe the appearance of the diffraction pattern on the film . ( b ) A flat photographic plate is placed behind ...
Page 94
... diffraction in crystals , imperfect crystals and amorphous bodies , Freeman , 1963 . W. C. Hamilton , " The revolution in crystallography , " Science 169 , 133 ( 1970 ) . K. C. Holmes and D. M. Blow , Use of x - ray diffraction in the ...
... diffraction in crystals , imperfect crystals and amorphous bodies , Freeman , 1963 . W. C. Hamilton , " The revolution in crystallography , " Science 169 , 133 ( 1970 ) . K. C. Holmes and D. M. Blow , Use of x - ray diffraction in the ...
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