A slice of AdS_5 as the large N limit of Seiberg duality

Abel, Steven; Gherghetta, Tony

doi:10.1007/JHEP12(2010)091

Article
Report number	arXiv:1010.5655 ; IPPP-10-86 ; DCPT-10-172 ; CERN-PH-TH-2010-234 ; IPPP-10-86 ; DCPT-10-172 ; CERN-PH-TH-2010-234
Title	A slice of AdS_5 as the large N limit of Seiberg duality
Author(s)	Abel, Steven (Durham U., IPPP ; CERN) ; Gherghetta, Tony (Melbourne U.)
Publication	2010
Imprint	28 Oct 2010
Number of pages	47
Note	Comments: 47 Pages, axodraw4j.sty 47 Pages, axodraw4j.sty
In:	JHEP 12 (2010) 091
DOI	10.1007/JHEP12(2010)091
Subject category	Particle Physics - Theory
Abstract	A slice of AdS_5 is used to provide a 5D gravitational description of 4D strongly-coupled Seiberg dual gauge theories. An (electric) SU(N) gauge theory in the conformal window at large N is described by the 5D bulk, while its weakly coupled (magnetic) dual is confined to the IR brane. This framework can be used to construct an N = 1 MSSM on the IR brane, reminiscent of the original Randall-Sundrum model. In addition, we use our framework to study strongly-coupled scenarios of supersymmetry breaking mediated by gauge forces. This leads to a unified scenario that connects the extra-ordinary gauge mediation limit to the gaugino mediation limit in warped space.
Copyright/License	Open Access Preprint: © 2010-2025 CERN (License: CC-BY-3.0)

$noimg: \emph{Spectrum and anomaly free charges in }SQCD\emph{.}: \emph{Spectrum and anomaly free charges in} $\overline{\mbox{SQCD}}$$ $\it Types of SQCD RG flow with $t=\log E$. The solid and dashed lines are the electric and magnetic theories and $\lambda=g^2 \nc$ or $\bar{g}^2 \nnc$ respectively. The undeformed theories flow to their conformal fixed points in (a). Upon adding a mass deformation the theories flow to new fixed points as in (b) or to IR-free theories as in (c). The magnetic theory was started at small coupling in order to show its evolution towards the unstable fixed point first $h_{* }=0$, $g_{* }$ before ending up at the stable fixed point $h_*^{\prime }$, $g_*^{\prime }$.$ $\it Types of SQCD RG flow with $t=\log E$. The solid and dashed lines are the electric and magnetic theories and $\lambda=g^2 \nc$ or $\bar{g}^2 \nnc$ respectively. The undeformed theories flow to their conformal fixed points in (a). Upon adding a mass deformation the theories flow to new fixed points as in (b) or to IR-free theories as in (c). The magnetic theory was started at small coupling in order to show its evolution towards the unstable fixed point first $h_{* }=0$, $g_{* }$ before ending up at the stable fixed point $h_*^{\prime }$, $g_*^{\prime }$.$ Show more plots

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Zapis kreiran 2010-10-28, zadnja izmjena 2023-10-04

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