Introduction to Solid State Physics |
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Page 328
... band every electron changes its k value at a rate given by hdk / dt = F , as derived above . The electrons are not ... band . ) If the band is filled except for an electron missing from the state E ( Fig . 11b ) , we say that there is a ...
... band every electron changes its k value at a rate given by hdk / dt = F , as derived above . The electrons are not ... band . ) If the band is filled except for an electron missing from the state E ( Fig . 11b ) , we say that there is a ...
Page 538
... bands are separated by an exchange interaction . The 3d ↑ band is filled ; the 3d ↓ band contains 4.46 electrons and 0.54 hole . The 4s band is usually thought to contain approximately equal numbers of electrons in both spin ...
... bands are separated by an exchange interaction . The 3d ↑ band is filled ; the 3d ↓ band contains 4.46 electrons and 0.54 hole . The 4s band is usually thought to contain approximately equal numbers of electrons in both spin ...
Page 658
... bands to the s band pro vided we take 0.54 more from one d sub - band than from the other d sub - band Evidence that our particular choice may correspond to reality is provided by Fig . 19 which shows the effect on the magneton number ...
... bands to the s band pro vided we take 0.54 more from one d sub - band than from the other d sub - band Evidence that our particular choice may correspond to reality is provided by Fig . 19 which shows the effect on the magneton number ...
Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
Copyright | |
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absolute zero absorption alkali halide alloy antiferromagnet applied field atoms axis boundary Brillouin zone calculated Chapter charge components conduction band conduction electrons crystal structure cubic density dielectric constant dielectric function diffraction dipole direction dislocation dispersion relation effective mass elastic electric field electron concentration electron gas energy gap equation equilibrium excited exciton experimental F center Fermi surface ferroelectric ferromagnetic Figure free electron frequency function given heat capacity hole impurity interaction ionic lattice constant lattice points low temperatures magnetic field magnetic moment magnon metal modes momentum motion nearest neighbors neutron normal nuclear optical orbital paramagnetic particle phase phonon Phys plane polarization positive potential primitive cell quantum reciprocal lattice vector region resonance result room temperature scattering semiconductor shown in Fig space specimen sphere superconducting theory thermal tion transition unit vacancy valence band velocity wavefunction wavelength wavevector x-ray