Dr Paul Kinsler. [Acknowledgements & Feedback]
This is part of a hyperlinked notes maze -- please read the index-file for important information about the nature and reliability of this document.
FK-phonons (Fuchs and Kliewer FK-1965 PR140) are interface phonon-polaritons, the decaying solutions to the (TO-phonon) transverse part of the phonon equations (see Babiker-1992) (WARNING: THIS IS NOT CERTAIN). Because they are transverse, their interaction with electrons is by an A.p interaction term (Babiker-1992 p B58). There seem to be no s-polarised interface phonons (mentioned in Babiker-Z-1998).
There are other "interface" (evanescent) phonons, corresponding to LO-phonons with k_L imaginary.
The FK-phonon mode displacements are
w_x = -i k_x ( e^{k_L z} \pm \exp^{-k_L z} ) e^{ i (k_x x - \omega t) }
w_z = - k_x ( e^{k_L z} \mp \exp^{-k_L z} ) e^{ i (k_x x - \omega t) }
\phi_{LO} = -\rho_{IP} ( e^{k_L z} \pm \exp^{-k_L z} ) e^{ i (k_x x - \omega t) }
OLD: These are phonons localised on interfaces between different layers. More specifically, this file deals with Fuchs and Kliewer interface phonons (FK-phonons), and not the decaying LO-phonon or TO-phonon modes that can be attached to interfaces when k_L or k_T is imaginary.
XINDEX: phonon-polariton, log-file, hybrid-phonon, TO-phonon, TFM-model, Ridley-B-1991, Ridley-ACB-1994, Ridley-1993, LO-phonon, HD-model, FK-phonon, Educato-LBVJ-1993, DC-model, Babiker-1992, index-file, log-file.
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Email Feedback: Dr.Paul.Kinsler@physics.org
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