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- adiabatic approximation
- Interatomic ForcesLattice Vibrations
- alkali halide crystals
- Problem: Optical Mode of
- Anderson model
- Problem: Anderson Model
- anharmonic effects
- Interatomic ForcesLattice Vibrations, Problem: Spontaneous Polarization, Problem: Divergent Susceptibility
- band gap
- Problem: Nearly Free Electrons
- band insulator
- Problem: Electrons in 2D , Problem: Electrons in 2D
- band metal
- Problem: Electrons in 2D , Problem: Electrons in 2D
- band overlap
- Problem: Band Overlap
- band structure
- one-dimensional
- Problem: Band Overlap
- quasi-two-dimensional
- Problem: Electronic Specific Heat
- square lattice
- Problem: Nearly Free Electrons
- bandwidth
- Problem: Dirac-Delta Potentials
- basis
- Crystal Structures, Problem: Copper Oxide Layers
- bcc
- seebody centered cubic structure
- BCS theory
- Problem: Density of States
- Bethe-Sommerfeld expansion
- Problem: Chemical Potential of
- bias voltage
- Problem: p-n Junctions
- binding energy
- Interatomic ForcesLattice Vibrations
- ionic
- Interatomic ForcesLattice Vibrations
- metallic
- Interatomic ForcesLattice Vibrations
- van der Waals
- Interatomic ForcesLattice Vibrations
- Bloch oscillations
- Problem: Bloch Oscillations
- body centered cubic structure
- Crystal Structures, Problem: hcp and bcc
- Boltzmann equation
- Problem: Conductivity of Tight-Binding , Problem: Hall Effect in , Problem: Free-Electron Results from , Problem: Frequency-Dependent Conductivity
- Bragg
- condition
- Crystal Structures
- Bravais lattice
- Crystal Structures, Problem: Copper Oxide Layers
- Brillouin zone
- Crystal Structures, Problem: Tight-Binding Band in
- buckyball
- seeC
- bulk modulus
- Interatomic ForcesLattice Vibrations, Problem: Temperature Dependence of
- NaCl
- Problem: NaCl Bulk Modulus
- C
- structure
- Problem: Structure of AC
- C
- structure factor
- Problem: Structure Factor of
- C
- Rb
C
Madelung constant - Problem: Madelung Constant
- charge density waves
- Problem: Density of States
- chemical potential
- Problem: Electron-Hole Symmetry, Problem: Chemical Potential of
- electron in a plane
- Problem: Quantum Hall Effect
- classical statistics
- Problem: Electron-Hole Symmetry
- cm
- seewavenumbers
-
-Co - Problem: Powder Diffraction of
-
-Co - Problem: Powder Diffraction of
- Cobalt
- Problem: Powder Diffraction of
- cohesive energy
- Interatomic ForcesLattice Vibrations
- ionic
- Interatomic ForcesLattice Vibrations
- metallic
- Interatomic ForcesLattice Vibrations
- van der Waals
- Interatomic ForcesLattice Vibrations
- compressibility
- Problem: Temperature Dependence of
- phonons
- Problem: Bulk Modulus of
- solids
- Interatomic ForcesLattice Vibrations
- conduction band
- Problem: Excitons, Problem: Direct-Gap Semiconductor
- conductivity
- Drude
- Problem: Frequency-Dependent Response of
- electrical
- Problem: Thermal Conductivity
- frequency-dependent
- Problem: Frequency-Dependent Conductivity
- isotropic
- Problem: Conductivity Tensor
- of a superconductor
- Problem: Frequency-Dependent Response of
- semiconductor
- Problem: Direct-Gap Semiconductor
- tensor
- Problem: Conductivity Tensor, Problem: Conductivity of Tight-Binding , Problem: Hall Effect in
- tensor
- Problem: Conductivity Tensor, Problem: Conductivity of Tight-Binding , Problem: Hall Effect in
- tensor
- Problem: Conductivity Tensor, Problem: Conductivity of Tight-Binding , Problem: Hall Effect in
- thermal
- Problem: Thermal Conductivity
- coordination number
- Crystal Structures
- copper
- Problem: Hybridization of Energy
- covalent solids
- (, )
- crystal
- Crystal Structures
- crystallographic point group
- Crystal Structures
- crystallographic space group
- Crystal Structures
- finite
- Problem: Finite Size Effects
- imperfect
- Problem: Random Displacement
- symmetry
- Crystal Structures
- crystal structure
- Crystal Structures
- diamond
- Problem: Inversion Symmetry
- crystallographic space groups
- Crystal Structures
- cyclotron effective mass
- Problem: Cyclotron Frequency
- cyclotron frequency
- Problem: Quantum Hall Effect
- de Haas-van Alphen oscillations
- Problem: de Haas-van Alphen
- Debye
- frequency
- Interatomic ForcesLattice Vibrations, Problem: Debye Frequency, Problem: Two-Dimensional Debye, Problem: Specific Heat of
- frequency
- Interatomic ForcesLattice Vibrations, Problem: Debye Frequency, Problem: Two-Dimensional Debye, Problem: Specific Heat of
- frequency
- Interatomic ForcesLattice Vibrations, Problem: Debye Frequency, Problem: Two-Dimensional Debye, Problem: Specific Heat of
- frequency
- Interatomic ForcesLattice Vibrations, Problem: Debye Frequency, Problem: Two-Dimensional Debye, Problem: Specific Heat of
- temperature
- Interatomic ForcesLattice Vibrations
- wavenumber
- Interatomic ForcesLattice Vibrations, Problem: Number of Phonons, Problem: Energy of the
- wavenumber
- Interatomic ForcesLattice Vibrations, Problem: Number of Phonons, Problem: Energy of the
- wavenumber
- Interatomic ForcesLattice Vibrations, Problem: Number of Phonons, Problem: Energy of the
- Debye approximation
- Interatomic ForcesLattice Vibrations, Problem: Bulk Modulus of
- density
- fcc lattice
- Problem: hcp and fcc
- hcp lattice
- Problem: hcp and fcc
- density of states
- Problem: Density of States, Problem: Quasi-One-Dimensional Metal, Problem: Crossover to Quasi-One-Dimensional , (, ), Problem: Saddle Point, Problem: Electronic Specific Heat
- energy gap
- Problem: Energy Gap
- hybridized bands
- Problem: Density of States
- infinite dimensions
- Problem: Infinite-Dimensional DOS
- superconductor
- Problem: Density of States
- tight-binding
- Problem: Infinite-Dimensional DOS
- two dimensions
- Problem: Two-Dimensional Density of
- diatomic chain
- Problem: Diatomic Chain
- dielectric function
- Problem: One-Dimensional Electron System, Problem: Screening of an , Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting
- insulators
- Problem: Polaritons
- diffraction peak
-
-dependence - Problem: Random Displacement
- height and width of
- Problem: Finite Size Effects
- integrated intensity of
- Problem: Integrated Scattering Intensity
- diffusion current
- electron
- Problem: p-n Junctions
- hole
- Problem: p-n Junctions
- diode
- Problem: p-n Junctions
- dipole moment
- Problem: Soft Optical Phonons, Problem: Soft Phonons Again
- Dirac-delta function
- Problem: Electrons in 2D , Problem: Dirac-Delta Potentials in
- discrete translational symmetry
- Crystal Structures
- dispersion relation
- Problem: Diatomic Chain
- Drude model
- Problem: Two-Charge-Carrier Drude Model, Problem: Conductivity of Tight-Binding , Problem: Hall Effect in , Problem: Free-Electron Results from , Problem: Transmission of a
- dynamical matrix
- Interatomic ForcesLattice Vibrations, Problem: Long Range Interaction
- Dyson-Maleev representation
- Problem: Dyson-Maleev Representation, Problem: Spin Waves Again
-
- seedielectric function
- effective mass
- cyclotron
- Problem: Cyclotron Frequency
- effective mass tensor
- Problem: Effective Mass, Problem: Cyclotron Frequency, Problem: Saddle Point, Problem: Electronic Specific Heat
- eigenfrequency
- Problem: Mass Defect
- Einstein model
- Interatomic ForcesLattice Vibrations
- electromagnetic waves
- Problem: Polaritons
- electron gas
- seefree-electron gas
- electron-electron interaction
- Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting
- infinite range
- Problem: Infinite Range Hubbard
- electron-phonon interaction
- Interatomic ForcesLattice Vibrations, Problem: Polarons
- electrons
- one-dimensional
- Problem: Energy Gap, Problem: Free Energy with , Problem: Peierls Distortion
- one-dimensional
- Problem: Energy Gap, Problem: Free Energy with , Problem: Peierls Distortion
- one-dimensional
- Problem: Energy Gap, Problem: Free Energy with , Problem: Peierls Distortion
- quasi-one-dimensional
- Problem: Quasi-One-Dimensional Metal, Problem: Crossover to Quasi-One-Dimensional , Problem: Bloch Oscillations, Problem: Fermi Surface Nesting
- quasi-one-dimensional
- Problem: Quasi-One-Dimensional Metal, Problem: Crossover to Quasi-One-Dimensional , Problem: Bloch Oscillations, Problem: Fermi Surface Nesting
- quasi-one-dimensional
- Problem: Quasi-One-Dimensional Metal, Problem: Crossover to Quasi-One-Dimensional , Problem: Bloch Oscillations, Problem: Fermi Surface Nesting
- quasi-one-dimensional
- Problem: Quasi-One-Dimensional Metal, Problem: Crossover to Quasi-One-Dimensional , Problem: Bloch Oscillations, Problem: Fermi Surface Nesting
- quasi-two-dimensional
- Problem: de Haas-van Alphen
- energy
- electrons
- Problem: Free Energy with
- energy band
- Problem: Instability at the , Problem: Quasi-One-Dimensional Metal, Problem: Electron-Hole Symmetry
- energy dispersion
- Problem: Diatomic Chain
- energy gap
- Problem: Dirac-Delta Potentials, Problem: Nearly Free Electrons , Problem: Density of States , Problem: Electron-Hole Symmetry
- direct
- Problem: Direct-Gap Semiconductor
- due to periodic potential
- Problem: Energy Gap
- entropy
- Problem: Entropy of the
- electron gas
- Problem: Free Energy with
- EuO
- specific heat
- Problem: EuO Specific Heat
- Ewald construction
- Crystal Structures
- exciton
- Problem: Excitons
- face centered cubic structure
- Crystal Structures, Problem: Powder Diffraction of
- Fermi energy
- Problem: Fermi Energy, Problem: Specific Heat of
- Fermi surface
- Problem: Electrons in 2D
- nesting of
- Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting
- nesting of
- Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting
- nesting of
- Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting , Problem: Fermi Surface Nesting
- square lattice
- Problem: Electrons in 2D
- ferromagnet
- Problem: Spin Waves, Problem: Anisotropic Heisenberg Model
- filling factor
- Crystal Structures
- finite size effect
- Problem: Finite Size Effects
- flux quantum
- Problem: Quantum Hall Effect
- form factor
- Crystal Structures
- Fourier transform infrared spectroscopy
- Problem: Fourier Transform Infrared
- free-electron gas
- bulk modulus
- Problem: Temperature Dependence of
- chemical potential
- Problem: Chemical Potential of
- entropy
- Problem: Entropy of the
- one-dimensional
- Problem: Instability at the
- three-dimensional
- Problem: Screening of an
- two-dimensional
- Problem: Two-Dimensional Electron Gas
- free-electron model
- Problem: Frequency-Dependent Response of
- Friedel oscillation
- Problem: Screening of an
- fullerenes
- seeC
- Grüneisen parameter
- Interatomic ForcesLattice Vibrations, Problem: Grüneisen Parameter
- Grüneisen relation
- Problem: Bulk Modulus of
- graphite
- Problem: Graphite
- group theory
- Crystal Structures
- Hall coefficient
- Problem: Two-Charge-Carrier Drude Model, Problem: Hall Effect in
- Hall effect
- quantum
- Problem: Quantum Hall Effect
- hcp
- seehexagonal close packed structure
- Heisenberg model
- Problem: Spin Waves, Problem: Spin Waves Again, Problem: Large-U Hubbard Model
- anisotropic
- Problem: Anisotropic Heisenberg Model
- hexagonal close packed structure
- Problem: Structure of AC, Problem: hcp and bcc , Problem: Powder Diffraction of
- hexagonal lattice
- Problem: Two-Dimensional Debye
- Fermi energy
- Problem: Fermi Energy
- high
superconductors - Problem: Copper Oxide Layers
- high
superconductors - Problem: Conductivity Tensor
- Holstein-Primakoff transformation
- Problem: Holstein-Primakoff Transformation
- honeycomb lattice
- Crystal Structures
- hopping conductivity
- Problem: Hybridization of Energy
- Hubbard model
- infinite range
- Problem: Infinite Range Hubbard
- large U
- Problem: Large-U Hubbard Model
- hybridization
- Problem: Density of States , Problem: Hybridization of Energy , Problem: Anderson Model
- infrared activity
- Problem: Inversion Symmetry
- infrared spectroscopy
- Problem: Fourier Transform Infrared , Problem: Inversion Symmetry
- infrared-activity
- Problem: Inversion Symmetry
- interaction
- electron-phonon
- Problem: Peierls Distortion
- interband transition
- Problem: Direct-Gap Semiconductor
- inversion symmetry
- Problem: Inversion Symmetry
- ionic solids
- (, )
- IR
- seeinfrared spectroscopy
- Ising model
- Problem: Spin Waves
- isotope substitution
- Problem: Mass Defect
- Kohn anomaly
- Problem: Fermi Surface Nesting
- Kramers-Kronig relation
- Problem: Frequency-Dependent Conductivity
- lattice
- seeBravais lattice
- lattice spacing
- Crystal Structures, Crystal Structures
- bcc
- Problem: hcp and bcc
- hcp
- Problem: hcp and bcc
- lattice vector
- Crystal Structures, Crystal Structures
- lattice vibration
- Interatomic ForcesLattice Vibrations
- Laue condition
- Crystal Structures
- Lennard-Jones potential
- Interatomic ForcesLattice Vibrations
- Lindemann melting formula
- Interatomic ForcesLattice Vibrations
- linear chain
- Problem: Soft Optical Phonons, Problem: Soft Phonons Again, Problem: Spontaneous Polarization, Problem: Divergent Susceptibility
- radiation from
- Problem: Linear Array of
- static modulation
- Problem: Linear Array of
- time dependent modulation
- Problem: Linear Array of
- vibrations of
- Problem: Mass Defect
- Linhard function
- Problem: One-Dimensional Electron System, Problem: Screening of an
- in d dimensions
- Problem: Singularity at
- localized mode
- Problem: Mass Defect
- longitudinal phonon
- Interatomic ForcesLattice Vibrations, Problem: Debye Frequency
- low-pass filters
- neutron
- Problem: Neutron Diffraction Device
- Lyddane-Sachs-Teller relation
- Problem: Polaritons, Problem: Polaritons
- Madelung constant
- Problem: Madelung Constant
- screened Coulomb potential
- Problem: Madelung with Screened
- Madelung energy
- Interatomic ForcesLattice Vibrations
- magnetic moment
- Problem: Stoner Model
- transition metals
- Problem: Anderson Model
- magnetization
- temperature dependence
- Problem: Magnetization at Low
- magnetoresistance
- Problem: Two-Charge-Carrier Drude Model
- magnon
- Problem: Spin Waves, Problem: EuO Specific Heat, Problem: Magnetization at Low
- majority current
- Problem: p-n Junctions
- mass defect
- Problem: Mass Defect
- Matthiessen rule
- Problem: Residual Resistivity
- mean field approximation
- Problem: Susceptibility of a , Problem: Critical Temperature in
- Anderson model
- Problem: Anderson Model
- Stoner model
- Problem: Stoner Model
- mean free path
- Problem: Frequency-Dependent Conductivity
- melting
- seeLindemann melting formula
- metal
- Interatomic ForcesLattice Vibrations
- two-dimensional
- Problem: Conductivity of Tight-Binding , Problem: Hall Effect in , Problem: Frequency-Dependent Conductivity
- two-dimensional
- Problem: Conductivity of Tight-Binding , Problem: Hall Effect in , Problem: Frequency-Dependent Conductivity
- two-dimensional
- Problem: Conductivity of Tight-Binding , Problem: Hall Effect in , Problem: Frequency-Dependent Conductivity
- Miller indices
- Crystal Structures
- minority current
- Problem: p-n Junctions
- mobility
- Problem: Two-Charge-Carrier Drude Model
- Montgomery method
- Problem: Montgomery Method
- NaCl
- Problem: NaCl Bulk Modulus
- NbSe
- Problem: Quasi-One-Dimensional Metal
- nearest-neighbor @;tex2html_html_special_mark_quot;interaction
- Problem: Diatomic Chain
- nearest-neighbor interaction
- Problem: Grüneisen Parameter
- nearly free-electron approximation
- Problem: Dirac-Delta Potentials, Problem: Nearly Free Electrons , Problem: Nearly Free Electron , Problem: Electrons in 2D , Problem: Dirac-Delta Potentials in
- neutron beam
- Problem: Neutron Diffraction Device
- neutron scattering
- Interatomic ForcesLattice Vibrations
- energy resolution
- Problem: Triple-axis Spectrometer
- momentum resolution
- Problem: Momentum Resolution
- nickel
- Problem: Hybridization of Energy
- one-dimensional chain
- Problem: Nearly Free Electrons , Problem: Tight-Binding in Dirac-Delta , Problem: Dirac-Delta Potentials
- optical conductivity
- insulators
- Problem: Polaritons
- optical phonon
- Problem: Inversion Symmetry
- soft
- Problem: Soft Optical Phonons, Problem: Soft Phonons Again
- soft
- Problem: Soft Optical Phonons, Problem: Soft Phonons Again
- optical spectroscopy
- Interatomic ForcesLattice Vibrations, Problem: Optical Mode of
- oscillator sum rule
- Problem: Frequency-Dependent Conductivity
- Peierls transition
- Problem: Peierls Distortion
- Peltier coefficient
- Problem: Thermal Conductivity
- penetration depth
- Problem: Frequency-Dependent Response of
- periodic potential
- Problem: Instability at the
- phonon
- Interatomic ForcesLattice Vibrations, Problem: Linear Array of
- acoustical
- Problem: Phonons in Silicon
- branch
- Interatomic ForcesLattice Vibrations
- dispersion
- Interatomic ForcesLattice Vibrations, Problem: Phonon Mode of
- dispersion
- Interatomic ForcesLattice Vibrations, Problem: Phonon Mode of
- energy
- Problem: Energy of the
- in one dimension
- Interatomic ForcesLattice Vibrations
- interaction
- Interatomic ForcesLattice Vibrations
- lifetime
- Interatomic ForcesLattice Vibrations
- number of
- Interatomic ForcesLattice Vibrations, Problem: Number of Phonons
- number of
- Interatomic ForcesLattice Vibrations, Problem: Number of Phonons
- one dimension
- Problem: Long Range Interaction
- optical
- Interatomic ForcesLattice Vibrations
- specific heat
- Problem: Energy of the
- spectrum
- Interatomic ForcesLattice Vibrations
- transverse
- Problem: Phonons in Silicon
- phonon dispersion
- Problem: Long Range Interaction
-
- seePeltier coefficient
- p-n junction
- Problem: p-n Junctions
- point charge impurity
- Problem: Screening of an
- polariton
- Problem: Polaritons, Problem: Spontaneous Polarization, Problem: Divergent Susceptibility
- polarizability
- Problem: Soft Optical Phonons, Problem: Soft Phonons Again, Problem: Spontaneous Polarization, Problem: Divergent Susceptibility
- polarization
- spontaneous
- Problem: Spontaneous Polarization
- static
- Problem: Spontaneous Polarization
- time-dependent
- Problem: Divergent Susceptibility
- vector
- Interatomic ForcesLattice Vibrations
- polaron
- Problem: Polarons
- powder diffraction
- Problem: Neutron Diffraction Device
- primitive cell
- Crystal Structures
- primitive vectors
- Crystal Structures
- quantum Hall effect
- Problem: Two-Dimensional Electron Gas, Problem: Quantum Hall Effect
- Raman spectroscopy
- Problem: Inversion Symmetry
- random atomic displacement
- Problem: Random Displacement
- reciprocal lattice
- Crystal Structures, Problem: Copper Oxide Layers
- reflectivity
- Problem: Fourier Transform Infrared
- reflectivity coefficient
- Problem: Frequency-Dependent Response of
- relaxation time
- Problem: Free-Electron Results from
- resistivity
- anisotropy
- Problem: Anisotropic Layer
- intrinsic semiconductor
- Problem: Electric and Heat
- metal
- Problem: Electric and Heat
- oscillations
- Problem: de Haas-van Alphen
- residual
- Problem: Residual Resistivity
- tensor
- Problem: Montgomery Method
- resolution
- infrared spectroscopy
- Problem: Fourier Transform Infrared
- Rietveld analysis
- Crystal Structures
- saddle point
- Problem: Saddle Point
- screening parameter
- Problem: Screening of an
- self-consistency condition
- Problem: Anderson Model
- semiconductor
- Problem: Excitons, Problem: Electron-Hole Symmetry, Problem: Two-Charge-Carrier Drude Model, Problem: Direct-Gap Semiconductor
- junction
- Problem: p-n Junctions
- silicon
- phonons
- Problem: Phonons in Silicon, Problem: Inversion Symmetry
- phonons
- Problem: Phonons in Silicon, Problem: Inversion Symmetry
- simple cubic structure
- Crystal Structures
- sodium
- Problem: hcp and bcc
- soft phonon
- Problem: Soft Optical Phonons, Problem: Soft Phonons Again
- solids
- covalent
- (, )
- covalent
- (, )
- ionic
- (, )
- ionic
- (, )
- van der Waals
- (, )
- van der Waals
- (, )
- solitons
- Problem: Solitons
- sound velocity
- Problem: Debye Frequency, Problem: Diatomic Chain, Problem: Two-Dimensional Debye
- space lattice
- seeBravais lattice
- specific heat
- Problem: Quasi-One-Dimensional Metal, Problem: EuO Specific Heat
- insulator
- Problem: Specific Heat of
- metal
- Problem: Specific Heat of
- phonon
- Problem: Energy of the
- solids
- Interatomic ForcesLattice Vibrations
- specific heat effective mass
- Problem: Electronic Specific Heat
- spectroscopy
- optical
- Problem: Optical Mode of
- spin density waves
- Problem: Density of States
- spin wave
- Problem: Spin Waves
- spontaneous polarization
- Problem: Spontaneous Polarization
- square lattice
- Problem: Vibrations of a , Problem: Nearly Free Electrons , Problem: Nearly Free Electron , Problem: Electrons in 2D , Problem: Tight-Binding Band in , Problem: Electrons in 2D , Problem: Dirac-Delta Potentials in , Problem: Effective Mass
- oscillations
- Problem: Vibrations of a
- Stoner model
- Problem: Infinite Range Hubbard , Problem: Stoner Model
- structure factor
- Crystal Structures
- C
- Problem: Structure Factor of
- superconductor
- Problem: Frequency-Dependent Response of , Problem: Transmission of a
- susceptibility
- Problem: Divergent Susceptibility
- divergence of
- Problem: Susceptibility of a
- magnetic
- Problem: Stoner Model
- temperature dependence
- Problem: Susceptibility of a
- symmetry group
- Crystal Structures
- crystallographic point group
- Crystal Structures
- crystallographic space group
- Crystal Structures
- TaS
- Problem: Quasi-One-Dimensional Metal
- thermal conductivity
- intrinsic semiconductor
- Problem: Electric and Heat
- metal
- Problem: Electric and Heat
- thermal expansion coefficient
- linear
- Interatomic ForcesLattice Vibrations
- thermoelectric transport
- Problem: Thermal Conductivity
- thermopower
- Problem: Thermal Conductivity
- tight-binding approximation
- Problem: Dirac-Delta Potentials, Problem: Tight-Binding Band in , Problem: Electrons in 2D , Problem: de Haas-van Alphen, Problem: Conductivity of Tight-Binding , Problem: Hall Effect in
- tight-binding band
- Problem: Effective Mass, Problem: Electronic Specific Heat
- tight-binding model
- Problem: Tight-Binding Model, Problem: Frequency-Dependent Conductivity, Problem: Large-U Hubbard Model
- transition temperature
- Problem: Susceptibility of a , Problem: Critical Temperature in
- transmisivity
- Problem: Fourier Transform Infrared
- transmission
- metal
- Problem: Transmission of a
- superconductor
- Problem: Transmission of a
- transverse phonon
- Interatomic ForcesLattice Vibrations, Problem: Debye Frequency
- triple-axis neutron spectrometer
- Problem: Triple-axis Spectrometer
- tunnel diode
- Problem: p-n Junctions
- two-electron excitations
- Problem: Tight-Binding Model
- unit cell
- Crystal Structures, Problem: Copper Oxide Layers
- vacancy
- Problem: Vacancies
- valence band
- Problem: Excitons, Problem: Direct-Gap Semiconductor
- van der Waals solids
- (, )
- van Hove singularity
- Problem: Density of States
- wave vector
- Crystal Structures
- wavenumbers
- Problem: Fourier Transform Infrared
- Wigner-Seitz cell
- Crystal Structures
- X-ray diffraction
- C
- Problem: Structure of AC
- Cobalt
- Problem: Powder Diffraction of
This document can be accessed on the World Wide Web at
"http//:solidstate.physics.sunysb.edu/book/prob/ ".
Laszlo Mihaly
Thu Oct 31 13:23:11 EST 1996
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