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@ARTICLE{Mitev:171519,
author = {Mitev, Vladimir and Pomoni, Elli},
title = {{T}he {E}xact {E}ffective {C}ouplings of 4{D} {N}=2 gauge
theories},
reportid = {DESY-2014-03320, DESY-14-091. HU-Mathematik-14-13.
HU-EP-14/23. arXiv:1406.3629},
year = {2014},
abstract = {The anomalous dimensions of operators in the purely gluonic
SU(2,1|2) sector of any planar conformal N=2 theory can be
read off from the N=4 SYM results by replacing the N=4
coupling constant by an interpolating function of the N=2
coupling constants, to which we refer to as the effective
coupling. For a large class of N=2 theories we compute the
weak coupling expansion of these functions as well as the
leading strong coupling term by employing supersymmetric
localization. Via Feynman diagrams, we interpret our results
as the relative (between N=2 and N=4) finite renormalization
of the coupling constant. Using the AdS/CFT dictionary, we
identify the effective couplings with the effective string
tensions of the corresponding gravity dual theories. Thus,
any observable in the SU(2,1|2) sector can be obtained from
its N=4 counterpart by replacing the N=4 coupling constant
by the universal, for a given theory, effective coupling.},
keywords = {supersymmetry: 4 (INSPIRE) / coupling constant:
renormalization (INSPIRE) / operator: anomalous dimension
(INSPIRE) / expansion: weak coupling (INSPIRE) /
renormalization: finite (INSPIRE) / gravitation: duality
(INSPIRE) / field theory: conformal (INSPIRE) / AdS/CFT
correspondence (INSPIRE) / gauge field theory (INSPIRE) /
string tension (INSPIRE)},
cin = {T},
cid = {I:(DE-H253)T-20120731},
pnm = {514 - Theoretical Particle Physics (POF2-514) / GATIS -
Gauge Theory as an Integrable System (317089)},
pid = {G:(DE-HGF)POF2-514 / G:(EU-Grant)317089},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)25 / PUB:(DE-HGF)15},
eprint = {1406.3629},
howpublished = {arXiv:1406.3629},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:1406.3629;\%\%$},
url = {https://bib-pubdb1.desy.de/record/171519},
}