One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model

This paper carries forward a series of articles describing our enterprise to construct a gauge equivalent for the θ-deformed non-commutative p^{-2} model originally introduced by Gurau et al. [Comm. Math. Phys. 287 (2009), 275-290]. It is shown that breaking terms of the form used by Vilar et al. [J...

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Main Authors: Daniel N. Blaschke, Arnold Rofner, René I.P. Sedmik
Format: Article
Language:English
Published: National Academy of Science of Ukraine 2010-05-01
Series:Symmetry, Integrability and Geometry: Methods and Applications
Subjects:
Online Access:http://dx.doi.org/10.3842/SIGMA.2010.037
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author Daniel N. Blaschke
Arnold Rofner
René I.P. Sedmik
author_facet Daniel N. Blaschke
Arnold Rofner
René I.P. Sedmik
author_sort Daniel N. Blaschke
collection DOAJ
description This paper carries forward a series of articles describing our enterprise to construct a gauge equivalent for the θ-deformed non-commutative p^{-2} model originally introduced by Gurau et al. [Comm. Math. Phys. 287 (2009), 275-290]. It is shown that breaking terms of the form used by Vilar et al. [J. Phys. A: Math. Theor. 43 (2010), 135401, 13 pages] and ourselves [Eur. Phys. J. C: Part. Fields 62 (2009), 433-443] to localize the BRST covariant operator (D^2θ^2D^2)^{-1} lead to difficulties concerning renormalization. The reason is that this dimensionless operator is invariant with respect to any symmetry of the model, and can be inserted to arbitrary power. In the present article we discuss explicit one-loop calculations, and analyze the mechanism the mentioned problems originate from.
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spelling doaj.art-352bef076d9947689c5d10a034e33a782022-12-22T01:02:27ZengNational Academy of Science of UkraineSymmetry, Integrability and Geometry: Methods and Applications1815-06592010-05-016037One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge ModelDaniel N. BlaschkeArnold RofnerRené I.P. SedmikThis paper carries forward a series of articles describing our enterprise to construct a gauge equivalent for the θ-deformed non-commutative p^{-2} model originally introduced by Gurau et al. [Comm. Math. Phys. 287 (2009), 275-290]. It is shown that breaking terms of the form used by Vilar et al. [J. Phys. A: Math. Theor. 43 (2010), 135401, 13 pages] and ourselves [Eur. Phys. J. C: Part. Fields 62 (2009), 433-443] to localize the BRST covariant operator (D^2θ^2D^2)^{-1} lead to difficulties concerning renormalization. The reason is that this dimensionless operator is invariant with respect to any symmetry of the model, and can be inserted to arbitrary power. In the present article we discuss explicit one-loop calculations, and analyze the mechanism the mentioned problems originate from.http://dx.doi.org/10.3842/SIGMA.2010.037noncommutative field theorygauge field theoriesrenormalization
spellingShingle Daniel N. Blaschke
Arnold Rofner
René I.P. Sedmik
One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model
Symmetry, Integrability and Geometry: Methods and Applications
noncommutative field theory
gauge field theories
renormalization
title One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model
title_full One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model
title_fullStr One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model
title_full_unstemmed One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model
title_short One-Loop Calculations and Detailed Analysis of the Localized Non-Commutative p^{-2} U(1) Gauge Model
title_sort one loop calculations and detailed analysis of the localized non commutative p 2 u 1 gauge model
topic noncommutative field theory
gauge field theories
renormalization
url http://dx.doi.org/10.3842/SIGMA.2010.037
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AT reneipsedmik oneloopcalculationsanddetailedanalysisofthelocalizednoncommutativep2u1gaugemodel