Electron-phonon interactions and Kohn anomalies: Difference between revisions
Jump to navigation
Jump to search
Line 16: | Line 16: | ||
<math>H = H^0_{el} + H^0_{ph} + H_{coul} + H_{int}</math> | <math>H = H^0_{el} + H^0_{ph} + H_{coul} + H_{int}</math> | ||
Where | Where | ||
<math>H^0_{el} = \sum_{k \sigma}</math> | |||
<math>H^0_{el} = \sum_{k \sigma}E_kc^\dagger_{k \sigma}c_{k \sigma}</math> | |||
<math>H^0_{ph} = \sum_{k \lamda}E_kc^\dagger_{k \sigma}c_{k \sigma}</math> | |||
<math>H^0_{el} = \sum_{k \sigma}E_kc^\dagger_{k \sigma}c_{k \sigma}</math> | |||
---- | ---- | ||
Revision as of 17:29, 12 December 2012
Electron-phonon interactions
Free electrons in lattice
Phonons: crystal vibrations
Lattice Vibration and Phonons in 1D
Acoustical and Optical Phonon in 3D
Derivation of Hamiltonian Electron-Phonon Coupling
The Hamiltonian for the electron-phonon interaction can be described as
Where
Failed to parse (unknown function "\lamda"): {\displaystyle H^0_{ph} = \sum_{k \lamda}E_kc^\dagger_{k \sigma}c_{k \sigma}}