Renormalization group method based on the ionization energy theory (Q2431308)
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| English | Renormalization group method based on the ionization energy theory |
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Renormalization group method based on the ionization energy theory (English)
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13 April 2011
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The paper summarizes the author's own research (2001--2010) on the generalization of Feynman's atomic hypothesis to quantum many-body systems (e.g. solids) following the lines of \textit{R. Shankar}'s formalism [``Renormalization-group approach to interacting fermions'', Rev. Mod. Phys. 66, No.~1, 129--192 (1994), \url{doi:10.1103/RevModPhys.66.129}]. The departure point is an idea that ionization energies of the solid constituent atoms determine how they attract or repel each other in the bulk. Technically, that amounts to establishing a relationship between the effective electron-electron Coulomb potential and a corresponding dressed electron-phonon interaction potential. A suitable modification (ionization energy based) of the Fermi-Dirac distribution is involved in the subsequent analysis of screened Coulomb potentials of the considered many-electron system, by means of the Thomas-Fermi theory. The author's main goal is to demonstrate that the standard renormalization group formalism (Gell-Mann-Low, Zinn-Justin) can be adopted to the new setting. Arguments are mostly heuristic and/or computational.
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renormalization group
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Feynman's atomic hypothesis
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solids
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crystals
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ionization energy
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electron-phonon interaction
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electron-electron interaction
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Fermi-Dirac statistics
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screened Coulomb potential
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dielectric functions
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dressed heat capacity
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