Introduction to Solid State Physics |
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Page 261
... specimen to specimen , whereas the resistivity caused by thermal motion is independent of the specimen . The resistivity ratio of a specimen is usually defined as the ratio of its resistivity at room temperature to its resistivity at ...
... specimen to specimen , whereas the resistivity caused by thermal motion is independent of the specimen . The resistivity ratio of a specimen is usually defined as the ratio of its resistivity at room temperature to its resistivity at ...
Page 516
... specimen is at the point a in the figure . If we magnetize the specimen isothermally in a 10,000 gauss field , then μgВ / kT1≈ 1 and the specimen is brought to point b . The total lattice entropy is assumed to be much smaller than the ...
... specimen is at the point a in the figure . If we magnetize the specimen isothermally in a 10,000 gauss field , then μgВ / kT1≈ 1 and the specimen is brought to point b . The total lattice entropy is assumed to be much smaller than the ...
Page 562
... specimen as a whole , the magnetic moment may be very much less than the saturation moment , and the application of ant external magnetic field may be required to saturate the specimen . The behavior observed in polycrystalline specimens ...
... specimen as a whole , the magnetic moment may be very much less than the saturation moment , and the application of ant external magnetic field may be required to saturate the specimen . The behavior observed in polycrystalline specimens ...
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