1991
DOI: 10.1103/physrevlett.66.3233
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Constructing the three-dimensional Gross-Neveu model with a large number of flavor components

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Cited by 84 publications
(76 citation statements)
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“…That this is indeed the case in d = 3 has only recently been proven using the renormalization group technique of constructive field theory [17].…”
Section: Introductionmentioning
confidence: 99%
“…That this is indeed the case in d = 3 has only recently been proven using the renormalization group technique of constructive field theory [17].…”
Section: Introductionmentioning
confidence: 99%
“…Regarding the first inclusion, we were surprised to find in the recent literature a combinatorial proof, with a flavor of loop-erased random walk, of the eminently classical Cayley-Hamilton theorem [37]. As for the second inclusion, there is a very nice explicit Fermionic proof [12] that, for a generic n × n matrix N, (tr N) k(n−1)+1 is in the ideal generated by the matrix elements of N k .…”
Section: Iii2 Chains And/or Loops?mentioning
confidence: 99%
“…Now algebraic combinatorialists might not be too impressed by this since one can readily rewrite formula (12) under the form given by Towber [40] or Singer [34]. So the series expansion of the formal inverse itself is not new.…”
Section: The Formal Inverse As a One-point Correlation Functionmentioning
confidence: 99%
“…It has also been argued [12]- [14] that the four dimensional Yukawa-φ 4 theory in 4 − ǫ dimensions represents the universality class of the Gross-Neveu model in dimensions between 2 and 4. The latter is also renormalizable only in the 1/N expansion [15,16] and the critical exponents have been computed to high order [17]- [19]. The O(N) model has one relevant coupling constant in the 4-dimensional theory, so the fixed point of order ǫ is automatically infrared stable and the phase transition is of second order.…”
mentioning
confidence: 99%