Introduction to Solid State PhysicsNew edition of the most widely-used textbook on solid state physics in the world. Describes how the excitations and imperfections of actual solids can be understood with simple models that have firmly established scope and power. The foundation of this book is based on experiment, application and theory. Several significant advances in the field have been added including high temperature superconductors, quasicrystals, nanostructures, superlattices, Bloch/Wannier levels, Zener tunneling, light-emitting diodes and new magnetic materials. |
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Page 102
... wave , but a standing wave . At the zone boundaries sKmaxa Sπ , whence = us = u exp ( IST ) = u ( − 1 ) 3 . ( 12 ) This is a standing wave : alternate atoms oscillate in opposite phases , because u , = ± 1 according to whether s is an ...
... wave , but a standing wave . At the zone boundaries sKmaxa Sπ , whence = us = u exp ( IST ) = u ( − 1 ) 3 . ( 12 ) This is a standing wave : alternate atoms oscillate in opposite phases , because u , = ± 1 according to whether s is an ...
Page 177
... wave . A wave that travels neither to the right nor to the left is a standing wave : it doesn't go anywhere . The time - independent state is represented by standing waves . We can form two different standing waves from the two ...
... wave . A wave that travels neither to the right nor to the left is a standing wave : it doesn't go anywhere . The time - independent state is represented by standing waves . We can form two different standing waves from the two ...
Page 274
... wave propagates with the phase velocity c / e1 / 2 . • € real and < 0. For w real , K is imaginary and the wave is damped with a characteristic length 1 / K . ⚫e complex . For w real , K is complex and the waves are damped in space ...
... wave propagates with the phase velocity c / e1 / 2 . • € real and < 0. For w real , K is imaginary and the wave is damped with a characteristic length 1 / K . ⚫e complex . For w real , K is complex and the waves are damped in space ...
Contents
PERIODIC ARRAYS OF ATOMS | 3 |
1 | 10 |
INDEX SYSTEM FOR CRYSTAL PLANES | 12 |
Copyright | |
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a₁ absolute zero alloys approximation atoms axis band edge Bloch Brillouin zone Chapter charge collision components conduction band conduction electrons crystal structure defined density dielectric diffraction dimensions direction dislocation dispersion relation displacement effective mass elastic electric field electron concentration electron gas energy gap equation equilibrium exciton factor Fermi level Fermi surface ferromagnetic Figure flux Fourier free electron frequency function germanium heat capacity hole impurity integral interaction ionic ions lattice constant lattice point layer low temperatures magnetic field magnetic moment metals modes momentum motion nearest-neighbor neutron normal optical orbital oscillator particle phase phonon plane polarization potential energy primitive cell quantum reciprocal lattice vector resonance result scattering semiconductor shown in Fig silicon solution space specimen sphere spin superconducting Table theory thermal tion transition unit valence band values velocity voltage volume wave wavefunction wavelength wavevector x-ray zone boundary