Introduction to Solid State Physics |
From inside the book
Results 1-3 of 65
Page 115
... equilibrium separation Ro if the parameters p , λ of the re- pulsive interaction are known . To convert to SI , replace q2 by q2 / 4π € 0 . The total lattice energy of the crystal of 2N ions at their equilibrium separa- tion Ro may be ...
... equilibrium separation Ro if the parameters p , λ of the re- pulsive interaction are known . To convert to SI , replace q2 by q2 / 4π € 0 . The total lattice energy of the crystal of 2N ions at their equilibrium separa- tion Ro may be ...
Page 226
... equilibrium . Without such mechanisms we may not speak of the phonons at one end of the crystal as being in thermal equilibrium at a temperature T2 and those at the other end in equilibrium at T1 . It is not sufficient for thermal con ...
... equilibrium . Without such mechanisms we may not speak of the phonons at one end of the crystal as being in thermal equilibrium at a temperature T2 and those at the other end in equilibrium at T1 . It is not sufficient for thermal con ...
Page 642
... equilibrium at temperature T : P = e ̄Ev / kBT , ( 1 ) where Ey is the energy required to take an atom from a ... equilibrium number n of vacancies is given by the ratio of vacant to filled sites : If n < N , then N n - = e - Ev / kBT n ...
... equilibrium at temperature T : P = e ̄Ev / kBT , ( 1 ) where Ey is the energy required to take an atom from a ... equilibrium number n of vacancies is given by the ratio of vacant to filled sites : If n < N , then N n - = e - Ev / kBT n ...
Contents
CRYSTAL STRUCTURE | 1 |
CRYSTAL DIFFRACTION AND THE RECIPROCAL LATTICE | 43 |
CRYSTAL BINDING | 95 |
Copyright | |
22 other sections not shown
Common terms and phrases
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