Introduction to Solid State PhysicsProblems after each chapter. |
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Page 104
... consider the forces acting on an element of length Ax . At one end of the element the strain is e ( x ) , and at the other end it is e ( x + Ax ) = e ( x ) + ( de / dx ) Ax = e ( x ) + ( ə2u / əx2 ) △ x , and so the resultant force ...
... consider the forces acting on an element of length Ax . At one end of the element the strain is e ( x ) , and at the other end it is e ( x + Ax ) = e ( x ) + ( de / dx ) Ax = e ( x ) + ( ə2u / əx2 ) △ x , and so the resultant force ...
Page 579
... consider explicity only magnetic energy , as the correspond- ing expressions for electric energy are obtained by appropriate tran- scription . Our treatment is simple and rather naive , but it leads to the correct results . PERMANENT ...
... consider explicity only magnetic energy , as the correspond- ing expressions for electric energy are obtained by appropriate tran- scription . Our treatment is simple and rather naive , but it leads to the correct results . PERMANENT ...
Page 581
... consider the behavior of a simple model . We consider a single electron with orbital quantum number L = 1 moving about a nucleus , the whole being placed in an inhomogeneous crystalline electric field . We omit electron spin from the ...
... consider the behavior of a simple model . We consider a single electron with orbital quantum number L = 1 moving about a nucleus , the whole being placed in an inhomogeneous crystalline electric field . We omit electron spin from the ...
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