1969
DOI: 10.1007/bf01645676
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Convergence of Bogoliubov's method of renormalization in momentum space

Abstract: Bogoliubov's method of renormalization is formulated in momentum space. The convergence of the renormalized Feynman integrand is proved by an application of the power counting theorem.

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Cited by 534 publications
(517 citation statements)
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“…In principle, it should be possible to implement in position space a natural variant of the BPHZ renormalization procedure [14,15,16]; the R-operation is a rather general method for subtracting divergences, whose mechanism is quite insensitive to the particular prescription for the subtractions. Moreover, it might be possible to adapt the reformulation of the BPHZ procedure in terms of Hopf algebras, due to Kreimer [17].…”
Section: Discussionmentioning
confidence: 99%
“…In principle, it should be possible to implement in position space a natural variant of the BPHZ renormalization procedure [14,15,16]; the R-operation is a rather general method for subtracting divergences, whose mechanism is quite insensitive to the particular prescription for the subtractions. Moreover, it might be possible to adapt the reformulation of the BPHZ procedure in terms of Hopf algebras, due to Kreimer [17].…”
Section: Discussionmentioning
confidence: 99%
“…A (correct) proof of the validity of Bogoliubov's method was finally given by Hepp [18] in 1966 and by Zimmermann [32] in 1969.…”
Section: The Extension Of Distributionsmentioning
confidence: 98%
“…(17), we expandS(q) and renormalization constants over trees using Eqs. (23), (31), (32) and (33). We replace products by convolutions ∇ according to Eq.…”
Section: The Renormalized Electron Propagatormentioning
confidence: 99%
“…Classical perturbation theory, like the inductive solution of any deterministic equation, is indexed by trees, whether QFT perturbation theory is indexed by more complicated "Feynman graphs", which contain the famous "loops" of anti-particles responsible for the ultraviolet divergences 5 . But the classical trees hidden inside QFT were revealed in many steps, starting with Zimmermann (which called them forests...) [18] through Gallavotti and many others, until Kreimer and Connes viewed them as generators of Hopf algebras [19,20,21]. Roughly speaking the trees were hidden because they are not just subgraphs of the Feynman graphs.…”
Section: Arxiv:07050705v1 [Hep-th] 4 May 2007mentioning
confidence: 99%