Script N = 1 theories and a geometric master field
Author(s) -
Rajesh Gopakumar
Publication year - 2003
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 - 10.1088/1126-6708/2003/05/033
Subject(s) - superpotential , mathematical physics , eigenvalues and eigenvectors , matrix (chemical analysis) , physics , scalar (mathematics) , riemann surface , gauge theory , quantum field theory , mathematics , combinatorics , supersymmetry , quantum mechanics , pure mathematics , geometry , chemistry , chromatography
We study the large $N$ limit of the class of U(N) ${\CN}=1$ SUSY gaugetheories with an adjoint scalar and a superpotential $W(\P)$. In each of thevacua of the quantum theory, the expectation values $\la$Tr$\Phi^p$$\ra$ aredetermined by a master matrix $\Phi_0$ with eigenvalue distribution$\rho_{GT}(\l)$. $\rho_{GT}(\l)$ is quite distinct from the eigenvaluedistribution $\rho_{MM}(\l)$ of the corresponding large $N$ matrix modelproposed by Dijkgraaf and Vafa. Nevertheless, it has a simple form on theauxiliary Riemann surface of the matrix model. Thus the underlying geometry ofthe matrix model leads to a definite prescription for computing$\rho_{GT}(\l)$, knowing $\rho_{MM}(\l)$.Comment: 16 pages; v2. Further elaboration in Sec. 5 on the relation between gauge and matrix eigenvalue distributions, v3: Minor change
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