BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories
Abstract We consider the 1/2 BPS circular Wilson loop in a generic N $$ \mathcal{N} $$ = 2 SU(N) SYM theory with conformal matter content. We study its vacuum expectation value, both at finite N and in the large-N limit, using the interacting matrix model provided by localization results. We single...
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Online Access: | http://link.springer.com/article/10.1007/JHEP08(2019)108 |
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doaj-f86c4f16477d4d91b88ebebcc23262972020-11-25T03:49:37ZengSpringerOpenJournal of High Energy Physics1029-84792019-08-012019815210.1007/JHEP08(2019)108BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theoriesM. Billò0F. Galvagno1A. Lerda2Dipartimento di Fisica, Università di TorinoDipartimento di Fisica, Università di TorinoI.N.F.N. — sezione di TorinoAbstract We consider the 1/2 BPS circular Wilson loop in a generic N $$ \mathcal{N} $$ = 2 SU(N) SYM theory with conformal matter content. We study its vacuum expectation value, both at finite N and in the large-N limit, using the interacting matrix model provided by localization results. We single out some families of theories for which the Wilson loop vacuum expectation values approaches the N $$ \mathcal{N} $$ = 4 result in the large-N limit, in agreement with the fact that they possess a simple holographic dual. At finite N and in the generic case, we explicitly compare the matrix model result with the field-theory perturbative expansion up to order g 8 for the terms proportional to the Riemann value ζ (5), finding perfect agreement. Organizing the Feynman diagrams as suggested by the structure of the matrix model turns out to be very convenient for this computation.http://link.springer.com/article/10.1007/JHEP08(2019)108Extended SupersymmetryWilson’t Hooft and Polyakov loopsSupersymmetric Gauge TheoryConformal Field Theory |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
M. Billò F. Galvagno A. Lerda |
spellingShingle |
M. Billò F. Galvagno A. Lerda BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories Journal of High Energy Physics Extended Supersymmetry Wilson ’t Hooft and Polyakov loops Supersymmetric Gauge Theory Conformal Field Theory |
author_facet |
M. Billò F. Galvagno A. Lerda |
author_sort |
M. Billò |
title |
BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories |
title_short |
BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories |
title_full |
BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories |
title_fullStr |
BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories |
title_full_unstemmed |
BPS wilson loops in generic conformal N $$ \mathcal{N} $$ = 2 SU(N) SYM theories |
title_sort |
bps wilson loops in generic conformal n $$ \mathcal{n} $$ = 2 su(n) sym theories |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2019-08-01 |
description |
Abstract We consider the 1/2 BPS circular Wilson loop in a generic N $$ \mathcal{N} $$ = 2 SU(N) SYM theory with conformal matter content. We study its vacuum expectation value, both at finite N and in the large-N limit, using the interacting matrix model provided by localization results. We single out some families of theories for which the Wilson loop vacuum expectation values approaches the N $$ \mathcal{N} $$ = 4 result in the large-N limit, in agreement with the fact that they possess a simple holographic dual. At finite N and in the generic case, we explicitly compare the matrix model result with the field-theory perturbative expansion up to order g 8 for the terms proportional to the Riemann value ζ (5), finding perfect agreement. Organizing the Feynman diagrams as suggested by the structure of the matrix model turns out to be very convenient for this computation. |
topic |
Extended Supersymmetry Wilson ’t Hooft and Polyakov loops Supersymmetric Gauge Theory Conformal Field Theory |
url |
http://link.springer.com/article/10.1007/JHEP08(2019)108 |
work_keys_str_mv |
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1724494328951209984 |