Higher-dimensional invariants in 6D super Yang-Mills theory

Abstract We exploit the 6D, N $$ \mathcal{N} $$ = (1, 0) and N $$ \mathcal{N} $$ = (1, 1) harmonic superspace approaches to construct the full set of the maximally supersymmetric on-shell invariants of the canonical dimension d = 12 in 6D, N $$ \mathcal{N} $$ = (1, 1) supersymmetric Yang-Mills (SYM)...

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Bibliographic Details
Main Authors: Serafim Buyucli, Evgeny Ivanov
Format: Article
Language:English
Published: SpringerOpen 2021-07-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP07(2021)190
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Summary:Abstract We exploit the 6D, N $$ \mathcal{N} $$ = (1, 0) and N $$ \mathcal{N} $$ = (1, 1) harmonic superspace approaches to construct the full set of the maximally supersymmetric on-shell invariants of the canonical dimension d = 12 in 6D, N $$ \mathcal{N} $$ = (1, 1) supersymmetric Yang-Mills (SYM) theory. Both single- and double-trace invariants are derived. Only four single-trace and two double-trace invariants prove to be independent. The invariants constructed can provide the possible counterterms of N $$ \mathcal{N} $$ = (1, 1) SYM theory at four-loop order, where the first double-trace divergences are expected to appear. We explicitly exhibit the gauge sector of all invariants in terms of N $$ \mathcal{N} $$ = (1, 0) gauge superfields and find the absence of N $$ \mathcal{N} $$ = (1, 1) supercompletion of the F 6 term in the abelian limit.
ISSN:1029-8479