Supersymmetry and Theory of Heavy-Fermions

dc.creatorPépin, C.
dc.creatorLavagna, M.
dc.date1997-09-24
dc.date.accessioned2026-07-07T09:12:13Z
dc.date.available2026-07-07T09:12:13Z
dc.descriptionWe propose a new approach to the Kondo lattice in order to describe simultaneously the Kondo effect and the local magnetism. This approach relies on an original representation of the $S=1/2$ impurity spin in which the different degrees of freedom are represented by fermionic as well as bosonic variables. The magnetic instability is found at $J_c/D =0.67$ in definite improvement compared to usual fermionic mean- field theories. The dynamical susceptibility contains an inelastic peak in addition to the standard Lindhard-type Fermi liquid contribution. The Fermi surface sum rule includes $n_c+1$ states corresponding to large Fermi surfaces.
dc.description4 pages, 3 figures, RevTeX
dc.identifierhttps://arxiv.org/abs/cond-mat/9709256
dc.identifierhttp://arxiv.org/abs/cond-mat/9709256
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/151948
dc.subjectStrongly Correlated Electrons
dc.titleSupersymmetry and Theory of Heavy-Fermions
dc.typetext

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