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- URN to cite this document:
- urn:nbn:de:bvb:355-epub-395600
- DOI to cite this document:
- 10.5283/epub.39560
Abstract
Just as photons are the quanta of light, plasmons are the quanta of orchestrated charge-density oscillations in conducting media. Plasmon phenomena in normal metals, superconductors, and doped semiconductors are often driven by long-wavelength Coulomb interactions. However, in crystals whose Fermi surface is comprised of disconnected pockets in the Brillouin zone, collective electron excitations ...
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