Introduction to Solid State Physics |
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Page 499
... susceptibility without specifying the system of units . Quite frequently a susceptibility is defined referred to unit mass or to a mole of the substance . The molar susceptibility is written as XM ; the magnetic moment per gram is ...
... susceptibility without specifying the system of units . Quite frequently a susceptibility is defined referred to unit mass or to a mole of the substance . The molar susceptibility is written as XM ; the magnetic moment per gram is ...
Page 520
... susceptibility by perhaps 75 percent . Detailed calculations and comparison with experiment for the alkali metals are reported by Silverstein . 14 The magnetic susceptibility is considerably higher for most transition metals ( with ...
... susceptibility by perhaps 75 percent . Detailed calculations and comparison with experiment for the alkali metals are reported by Silverstein . 14 The magnetic susceptibility is considerably higher for most transition metals ( with ...
Page 530
... susceptibility is given by the Curie law X , = C / T , where C is the Curie constant . Using ( 1 ) and ( 2 ) , MT = C ( Ba + XM ) and ( CGS ) M x = = C Ba ( T — CX ) Χρ ( 3 ) The susceptibility has a singularity at T = CA. At this ...
... susceptibility is given by the Curie law X , = C / T , where C is the Curie constant . Using ( 1 ) and ( 2 ) , MT = C ( Ba + XM ) and ( CGS ) M x = = C Ba ( T — CX ) Χρ ( 3 ) The susceptibility has a singularity at T = CA. At this ...
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