Perturbative linearization of supersymmetric Yang-Mills theory

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dc.identifier.uri Ananth, Sudarshan Lechtenfeld, Olaf Malcha, Hannes Nicolai, Hermann Pandey, Chetan Pant, Saurabh 2021-03-31T06:01:23Z 2021-03-31T06:01:23Z 2020
dc.identifier.citation Ananth, S.; Lechtenfeld, O.; Malcha, H.; Nicolai, H.; Pandey, C. et al.: Perturbative linearization of supersymmetric Yang-Mills theory. In: Journal of High Energy Physics (JHEP) 2020 (2020), Nr. 10, 199. DOI:
dc.description.abstract Supersymmetric gauge theories are characterized by the existence of a transformation of the bosonic fields (Nicolai map) such that the Jacobi determinant of the transformation equals the product of the Matthews-Salam-Seiler and Faddeev-Popov determinants. This transformation had been worked out to second order in the coupling constant. In this paper, we extend this result (and the framework itself) to third order in the coupling constant. A diagrammatic approach in terms of tree diagrams, aiming to extend this map to arbitrary orders, is outlined. This formalism bypasses entirely the use of anti-commuting variables, as well as issues concerning the (non-)existence of off-shell formulations for these theories. It thus offers a fresh perspective on supersymmetric gauge theories and, in particular, the ubiquitous N = 4 theory. © 2020, The Author(s). eng
dc.language.iso eng
dc.publisher Berlin [u.a.] : Springer
dc.relation.ispartofseries Journal of High Energy Physics (JHEP) 2020 (2020), Nr. 10
dc.rights CC BY 4.0 Unported
dc.subject extended supersymmetry eng
dc.subject field theories in higher dimensions eng
dc.subject Gauge symmetry eng
dc.subject supersymmetric Gauge Theory eng
dc.subject.ddc 530 | Physik ger
dc.title Perturbative linearization of supersymmetric Yang-Mills theory
dc.type Article
dc.type Text
dc.relation.essn 1029-8479
dc.relation.issn 1126-6708
dc.bibliographicCitation.issue 10
dc.bibliographicCitation.volume 2020
dc.bibliographicCitation.firstPage 199
dc.description.version publishedVersion
tib.accessRights frei zug�nglich

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