Abstract
A geometrical non-Abelian bosonization for the Fermi surface excitations is constructed. We introduce a unitary operator which generates the deformation of the Fermi surface which obeys non-Abelian Kac-Moody-Poisson brackets. We study the Hubbard model for d\ensuremath{\ge}1, the charge part is a Fermi liquid at finite temperature and a Luttinger liquid for d=1 at T=0. The spin part is described by an 0(3) nonlinear sigma model. \textcopyright{} 1996 The American Physical Society.
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