A simple form of the exact renormalization group method is proposed for the study of supersymmetric gauge field theory. The method relies on the existence of ultraviolet-finite four dimensional gauge theories with extended supersymmetry. The resulting exact renormalization group equation crucially depends on the Konishi anomaly of N=1 super Yang–Mills. We illustrate our method by dealing with the NSVZ exact relation for the beta functions, the N=2 super Yang–Mills effective potential and the N=1 super Yang–Mills gluon superpotential (the so-called Veneziano–Yankielowicz potential).
%0 Journal Article
%1 Arnone:2004ey
%A Arnone, S.
%A Yoshida, K.
%D 2004
%J Int. J. Mod. Phys.
%K GaugeTheory RGFlow SYM Supersymmetry VYeffectiveaction
%P 469-478
%R 10.1142/S0217979204024082
%T Application of exact renormalization group techniques to
the non-perturbative study of supersymmetric field
theory
%U http://www.slac.stanford.edu/spires/find/hep/www?j=IMPAE,B18,469
%V B18
%X A simple form of the exact renormalization group method is proposed for the study of supersymmetric gauge field theory. The method relies on the existence of ultraviolet-finite four dimensional gauge theories with extended supersymmetry. The resulting exact renormalization group equation crucially depends on the Konishi anomaly of N=1 super Yang–Mills. We illustrate our method by dealing with the NSVZ exact relation for the beta functions, the N=2 super Yang–Mills effective potential and the N=1 super Yang–Mills gluon superpotential (the so-called Veneziano–Yankielowicz potential).
@article{Arnone:2004ey,
abstract = {A simple form of the exact renormalization group method is proposed for the study of supersymmetric gauge field theory. The method relies on the existence of ultraviolet-finite four dimensional gauge theories with extended supersymmetry. The resulting exact renormalization group equation crucially depends on the Konishi anomaly of N=1 super Yang–Mills. We illustrate our method by dealing with the NSVZ exact relation for the beta functions, the N=2 super Yang–Mills effective potential and the N=1 super Yang–Mills gluon superpotential (the so-called Veneziano–Yankielowicz potential).},
added-at = {2009-04-24T14:01:22.000+0200},
author = {Arnone, S. and Yoshida, K.},
biburl = {https://www.bibsonomy.org/bibtex/281bf78dcbd44719024ee73b880a7002a/gber},
description = {SPIRES-HEP: FIND J IMPAE,B18,469},
doi = {10.1142/S0217979204024082},
interhash = {f582be556ac6a6306bb23d53012501ba},
intrahash = {81bf78dcbd44719024ee73b880a7002a},
journal = {Int. J. Mod. Phys.},
keywords = {GaugeTheory RGFlow SYM Supersymmetry VYeffectiveaction},
pages = {469-478},
slaccitation = {%%CITATION = IMPAE,B18,469;%%},
timestamp = {2009-04-24T14:01:22.000+0200},
title = {{Application of exact renormalization group techniques to
the non-perturbative study of supersymmetric field
theory}},
url = {http://www.slac.stanford.edu/spires/find/hep/www?j=IMPAE,B18,469},
volume = {B18},
year = 2004
}