Electron-phonon interactions and Kohn anomalies: Difference between revisions
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Where | Where | ||
<math>H^0_{el} = \sum_{k \sigma} | <math>H^0_{el} = \sum_{k \sigma}E_k c^\dagger_{k \sigma} c_{k \sigma}</math> | ||
<math>H^0_{ph} = \sum_{k \ | |||
<math>H^0_{ph} = \sum_{k \lambda}\omega_{k \lambda} a^\dagger_{k \lambda} + \frac{1}{2}</math> | |||
<math>H^0_{el} = \sum_{k \sigma}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 17:33, 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