1990
DOI: 10.1016/0370-2693(90)90425-6
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Four-fermi interaction in (2+1) dimensions beyond leading order in 1/N

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Cited by 47 publications
(37 citation statements)
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“…After performing the renormalization procedure [3,8,9], we can obtain the physical mass spectra ' -z r p ) . (o,o;o)( $$) mf -* *,*,G where we have used Z+= 1 to leading order [13]. This is in agreement with the result in the large-N expansion [4].…”
Section: R[+]= W [ J ] I Ddx (Rj(x)$c(x)+~(x)rl~x)+[~c(x)$c~x)+~(x)lsupporting
confidence: 83%
“…After performing the renormalization procedure [3,8,9], we can obtain the physical mass spectra ' -z r p ) . (o,o;o)( $$) mf -* *,*,G where we have used Z+= 1 to leading order [13]. This is in agreement with the result in the large-N expansion [4].…”
Section: R[+]= W [ J ] I Ddx (Rj(x)$c(x)+~(x)rl~x)+[~c(x)$c~x)+~(x)lsupporting
confidence: 83%
“…The natural counterparts of the bosonic models we have discussed are theories with four-Fermi interactions and U(N) symmetry, powercounting renormalizable in two dimensions and 1/N expandable. These theories are ultraviolet renormalizable order by order in the 1/N expansion in less than four dimensions, as shown by Rosenstein and coworkers [179][180][181] and by Kikukawa and Yamawaki [182], essentially because their ultraviolet limit has the same relevant operator content as the infrared limit of the superrenormalizable Yukawa model. These arguments were further developed in Refs.…”
Section: Fermionic Modelsmentioning
confidence: 84%
“…We believe that the next-toleading-order computation both demonstrates the renormalizability of the-four-~ermi theory and provides an aid in estimating the radius of convergence of the large-N expansion. There is a previous result on the renormaliza-tion in large-N with a single four-Fermi coupling and without further coupling to electromagnetic interactions [28]. There it is asserted that an additive renormalization of the auxiliary scalar fields of the model is necessary.…”
Section: Introductionmentioning
confidence: 97%