Introduction to Solid State Physics |
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Page 99
... absolute zero are summarized in Table 2 . The crystals are transparent insulators and are weakly bound , with low melting temperatures . The crystals are composed of atoms which have very high ioniza- tion energies ( see Table 3 ) . The ...
... absolute zero are summarized in Table 2 . The crystals are transparent insulators and are weakly bound , with low melting temperatures . The crystals are composed of atoms which have very high ioniza- tion energies ( see Table 3 ) . The ...
Page 109
Charles Kittel. Cohesive Energy The cohesive energy of inert gas crystals at absolute zero and at zero pres- sure is obtained by substituting ( 6 ) and ( 8 ) in ( 5 ) : 12 Utot ( R ) = 2.Ne [ ( 12.13 ) ( a ) 12 - ( 14.45 ) ...
Charles Kittel. Cohesive Energy The cohesive energy of inert gas crystals at absolute zero and at zero pres- sure is obtained by substituting ( 6 ) and ( 8 ) in ( 5 ) : 12 Utot ( R ) = 2.Ne [ ( 12.13 ) ( a ) 12 - ( 14.45 ) ...
Page 244
... absolute zero , and some levels are vacant which were occupied at absolute zero . The situation is illustrated by Fig . 4 , where the plotted curves are of the function 1 f ( e ) = e ( c - μ ) / kBT +1 ( 7 ) This is the Fermi - Dirac ...
... absolute zero , and some levels are vacant which were occupied at absolute zero . The situation is illustrated by Fig . 4 , where the plotted curves are of the function 1 f ( e ) = e ( c - μ ) / kBT +1 ( 7 ) This is the Fermi - Dirac ...
Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
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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