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 36
... result of the theory of elastic scattering of waves in a periodic lattice . If G is a reciprocal lattice vector , so ... result of Problem 1 is that the spacing d ( hkl ) between parallel lattice planes that are normal to the direction G ...
... result of the theory of elastic scattering of waves in a periodic lattice . If G is a reciprocal lattice vector , so ... result of Problem 1 is that the spacing d ( hkl ) between parallel lattice planes that are normal to the direction G ...
Page 232
... result agrees with ( 34 ) when = π / 2 . The result is in CGS ; to obtain SI , omit the c . = 5. Magnetoresistance with two carrier types . Problem 6.9 shows that in the drift veloc- ity approximation the motion of charge carriers in ...
... result agrees with ( 34 ) when = π / 2 . The result is in CGS ; to obtain SI , omit the c . = 5. Magnetoresistance with two carrier types . Problem 6.9 shows that in the drift veloc- ity approximation the motion of charge carriers in ...
Page 339
... result if we limit ourselves to long thin specimens with long axis parallel to Ba ; now the demagnetizing field contribution ( see Chapter 13 ) to B will be negligible , whence : * M ( CGS ) B = Вa + 4πM = 0 ; = or а Ba 1 4π ( 1 ) M 1 ...
... result if we limit ourselves to long thin specimens with long axis parallel to Ba ; now the demagnetizing field contribution ( see Chapter 13 ) to B will be negligible , whence : * M ( CGS ) B = Вa + 4πM = 0 ; = or а Ba 1 4π ( 1 ) M 1 ...
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