Introduction to Solid State PhysicsProblems after each chapter. |
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Page 173
... possible to determine the position of hydrogen atoms in a crystal by using x - rays , because of the low scatter- ing power of hydrogen . Neutron diffraction is a possible tool , especially if deu- terium is substituted for hydrogen ...
... possible to determine the position of hydrogen atoms in a crystal by using x - rays , because of the low scatter- ing power of hydrogen . Neutron diffraction is a possible tool , especially if deu- terium is substituted for hydrogen ...
Page 400
... possible for a structure with singly charged current carriers controlled by a potential hill . The properties of p - n junctions permit junction transistors to operate at very low voltage . In fact , a voltage of one or two tenths . of ...
... possible for a structure with singly charged current carriers controlled by a potential hill . The properties of p - n junctions permit junction transistors to operate at very low voltage . In fact , a voltage of one or two tenths . of ...
Page 490
... possible for the assembly to be displaced relative to the framework if there is a net flow of vacancies from one side to the other . This is possible if the specimen contains a concentration gradient allowing vacancies to enter one side ...
... possible for the assembly to be displaced relative to the framework if there is a net flow of vacancies from one side to the other . This is possible if the specimen contains a concentration gradient allowing vacancies to enter one side ...
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 levels 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 region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero