Introduction to Solid State PhysicsProblems after each chapter. |
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Page 242
... room temperature the values observed are in quite good agreement with the theoretical value given in ( 10.22 ) , as shown in Table 10.2 . The Lorenz number of pure copper at liquid hydrogen temperature ( ~ 15 ° K ) is an order of ...
... room temperature the values observed are in quite good agreement with the theoretical value given in ( 10.22 ) , as shown in Table 10.2 . The Lorenz number of pure copper at liquid hydrogen temperature ( ~ 15 ° K ) is an order of ...
Page 381
... room temperature . This behavior requires both donor and acceptor states to be produced , but the effect of the states depends on the position of the Fermi level . James and Lark - Horovitz 25 have proposed that each vacancy gives two ...
... room temperature . This behavior requires both donor and acceptor states to be produced , but the effect of the states depends on the position of the Fermi level . James and Lark - Horovitz 25 have proposed that each vacancy gives two ...
Page 459
... room temperature as the normal metals at room temperature . For exam- ple ; titanium , zirconium , and hafnium have resistivities at room tem- perature of 89 , 45 , and 32 microhm - cm , respectively , while copper , silver , and gold ...
... room temperature as the normal metals at room temperature . For exam- ple ; titanium , zirconium , and hafnium have resistivities at room tem- perature of 89 , 45 , and 32 microhm - cm , respectively , while copper , silver , and gold ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero