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Holographic Duals of FlavoredN=1 Super Yang-Mills: Beyond the Probe Approximation
Author(s) -
Benjamin A. Burrington,
James T. Liu,
Leopoldo A. Pando Zayas,
Diana Vaman
Publication year - 2005
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2005/02/022
Subject(s) - warp drive , physics , supergravity , conifold , brane cosmology , scalar (mathematics) , supersymmetry , gauge theory , dual polyhedron , theoretical physics , fundamental representation , yang–mills existence and mass gap , supersymmetry breaking , brane , mathematical physics , moduli space , particle physics , quantum mechanics , geometry , mathematics , lie algebra , weight
We construct backreacted D3/D7 supergravity backgrounds which are dual to four-dimensional N = 1 and N = 2 supersymmetric Yang-Mills at large Nc with flavor quarks in the fundamental representation of SU (Nc). We take into account the backreaction of D7-branes on either AdS 5 × S5 or AdS 5 × T1,1, or more generically on backgrounds where the space transverse to the D3-branes is Kähler. The construction of the backreacted geometry splits into two stages. First we determine the modification of the six-dimensional space transverse to the D3 due to the D7, and then we compute the warp factor due to the D3. The N = 2 background corresponds to placing a single stack of Nf D7-branes in AdS 5 × S5. Here the Kähler potential is known exactly, while the warp factor is obtained in certain limits as a perturbative expansion. By placing another D7 ′ probe in the backreacted D3/D7 background, we derive the effect of the D7-branes on the spectrum of the scalar fluctuations to first order in Nf. The two systems with N = 1 supersymmetry that we discuss are D3/D7/D7' and D3/D7 on the conifold. In both cases, the Kähler potential is obtained perturbatively in the number of D7-branes. We provide all the ingredients necessary for the computation of each term in the expansion, and in each case give the first few terms explicitly. Finally, we comment on some aspects of the dual gauge theories

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