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Renormalization of gauge invariant operators and anomalies in Yang-Mills theory
High Energy Physics - Theory · Submitted 29 Dec 1993
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A long-standing conjecture on the structure of renormalized, gauge invariant, integrated operators of arbitrary dimension in Yang-Mills theory is established.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
A long-standing conjecture on the structure of renormalized, gauge invariant, integrated operators of arbitrary dimension in Yang-Mills theory is established. The general solution of the consistency condition for anomalies with sources included is also derived. This is achieved by computing explicitely the cohomology of the full unrestricted BRST operator in the space of local polynomial functionals with ghost number equal to zero or one. The argument does not use power counting and is purely cohomological. It relies crucially on standard properties of the antifield formalism.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A long-standing conjecture on the structure of renormalized, gauge invariant, integrated operators of arbitrary dimension in Yang-Mills theory is established. | result 0.86 | 0.90 | 0.81 | asserted 1.00 |
| s1 | The general solution of the consistency condition for anomalies with sources included is also derived. | result 0.94 | 0.94 | 0.18 | asserted 1.00 |
| s2 | This is achieved by computing explicitely the cohomology of the full unrestricted BRST operator in the space of local polynomial functionals with ghost number equal to zero or one. | method 1.00 | 0.94 | 0.08 | asserted 1.00 |
| s3 | The argument does not use power counting and is purely cohomological. | method 0.93 | 0.87 | 0.04 | asserted 1.00 |
| s4 | It relies crucially on standard properties of the antifield formalism. | method 0.96 | 0.52 | 0.03 | asserted 1.00 |
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The paper
Original abstract
A long-standing conjecture on the structure of renormalized, gauge invariant, integrated operators of arbitrary dimension in Yang-Mills theory is established. The general solution of the consistency condition for anomalies with sources included is also derived. This is achieved by computing explicitely the cohomology of the full unrestricted BRST operator in the space of local polynomial functionals with ghost number equal to zero or one. The argument does not use power counting and is purely cohomological. It relies crucially on standard properties of the antifield formalism.
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References
How the literature uses it
6 arXiv papers cite this in 9 sentences
Papers citing it · 7 sentences without a confident label
Uses its method or tool 2 papers
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This relies on the evaluation of the cohomology $H_F(S_0)$ [ref] of the nilpotent operator $S_0$ in the space $F$ of Lorentz- and global $SU(2)$-invariant local functionals with dimension bounded by the power-counting. $H_F(S_0)$ is defined as the quotient of the latter functional space w.r.t. to the equivalence relation
Ambiguity-free formulation of the Higgs-Kibble model · Recursive Removal of the UV Divergences · 0.94
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One way to solve this problem is to compute the cohomology $H_F(S_0)$ [ref] of the nilpotent operator $S_0$ in the space $F$ of Lorentz- and global $SU(2)$-invariant local functionals with dimension bounded by the power-counting. $H_F(S_0)$ is defined as the quotient of the latter functional space w.r.t. to the equivalence relation
Renormalization of the Yang-Mills theory in the ambiguity-free gauge · Solution of the Linearized Functional Identity · 0.90
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