1973
DOI: 10.1007/bf01029302
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Ations of motion for a Legendre transform arbitrary order

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Cited by 29 publications
(22 citation statements)
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“…Since W V is composed of all connected graphs, including those containing higher order cumulants of W 0 , we see that the terms · · · Γ (2) 0 W V Γ (2) 0 · · · appearing in the iteration produce those unusual terms of the form W An alternative approach is the analog of the Dyson Schwinger equation for the effective action [35,52,53], reviewed in [5, sec. 1.8, 6.2].…”
Section: Discussionmentioning
confidence: 99%
“…Since W V is composed of all connected graphs, including those containing higher order cumulants of W 0 , we see that the terms · · · Γ (2) 0 W V Γ (2) 0 · · · appearing in the iteration produce those unusual terms of the form W An alternative approach is the analog of the Dyson Schwinger equation for the effective action [35,52,53], reviewed in [5, sec. 1.8, 6.2].…”
Section: Discussionmentioning
confidence: 99%
“…We mention here that the diagrams of φ (n) is obtained by attaching a black dot, in all possible ways, to one of the lines in the graphs of the n-th order of W . For example, the 31 diagrams of φ (4) is obtained through the fourth order of W ;…”
Section: Rule For J (N)mentioning
confidence: 99%
“…Note here that 1VI can not be replaced by 2PI (2-particle-irreducible) as in the case of the effective action for the non-local operator ϕ(x)ϕ(y) [2,4,6]. This is clear from the second and third (1VI) graphs from the last on the left-hand side of (2.40), which are 2PR (2-particlereducible).…”
Section: Rule For J (N)mentioning
confidence: 99%
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