Abstract
Collective transport phenomena are among the most fascinating properties in solid state physics. The best known example is superconductivity where the energy gap in the excitations at the Fermi level, as found by BCS [1] does not prevent conductivity. This is so because the interaction involved does not require a specific reference frame and because Cooper pairs can be built either in states “k and-k” of “k+κ or -k+ κ”. The latter state leads to a uniform velocity such as:
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Monceau, P. (1996). Introduction to Charge Density Wave Transport. In: Schlenker, C., Dumas, J., Greenblatt, M., van Smaalen, S. (eds) Physics and Chemistry of Low-Dimensional Inorganic Conductors. NATO ASI Series, vol 354. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-1149-2_24
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DOI: https://doi.org/10.1007/978-1-4613-1149-2_24
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