Introduction to Solid State Physics |
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Page 109
... quantum correction . We can under- stand the origin of the quantum correction by consideration of a simple model in which an atom is confined by fixed boundaries . If the particle has the quantum wavelength A , where A is determined by ...
... quantum correction . We can under- stand the origin of the quantum correction by consideration of a simple model in which an atom is confined by fixed boundaries . If the particle has the quantum wavelength A , where A is determined by ...
Page 241
... quantum theory and of the Pauli principle . Consider an electron of mass m confined to a length L by infinite barriers ( Fig . 2 ) . The wave- function ( x ) of the electron is a solution of the Schrödinger equation Hey ; with the ...
... quantum theory and of the Pauli principle . Consider an electron of mass m confined to a length L by infinite barriers ( Fig . 2 ) . The wave- function ( x ) of the electron is a solution of the Schrödinger equation Hey ; with the ...
Page 542
... quantum number of a system of N spins S are NS , NS − 1 , NS - 2 , ... , according to the quantum mechanics of angular momenta . In the ferromagnetic ground state the total spin quantum number has the value NS : all spins are parallel ...
... quantum number of a system of N spins S are NS , NS − 1 , NS - 2 , ... , according to the quantum mechanics of angular momenta . In the ferromagnetic ground state the total spin quantum number has the value NS : all spins are parallel ...
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