Introduction to Solid State Physics |
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Page 88
... values of Ak = k ' – k for which diffracted beams are found . First : We choose a set of translation vectors a , b , c for the assumed struc- ture . The vectors need not necessarily be primitive translation vectors . From a , b , c we ...
... values of Ak = k ' – k for which diffracted beams are found . First : We choose a set of translation vectors a , b , c for the assumed struc- ture . The vectors need not necessarily be primitive translation vectors . From a , b , c we ...
Page 120
... values of the repulsive parameters λ and p are very sensitive to the values of the input data B and Rọ , but the cohesive energy turns out to be relatively insensitive19 to the value adopted for p . The calcu- lated values of the ...
... values of the repulsive parameters λ and p are very sensitive to the values of the input data B and Rọ , but the cohesive energy turns out to be relatively insensitive19 to the value adopted for p . The calcu- lated values of the ...
Page 288
... values of the Hall constant for the mono- valent metals sodium and potassium are in excellent agreement with the values calculated for one valence electron per atom , using ( 42 ) . Notice next the values for the trivalent elements ...
... values of the Hall constant for the mono- valent metals sodium and potassium are in excellent agreement with the values calculated for one valence electron per atom , using ( 42 ) . Notice next the values for the trivalent elements ...
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