Gravitational corrections in supersymmetric gauge theory and matrix models
By A. Klemm, Marcos Mariño, S. Theisen. 2002
164 citations recorded by the source corpus.
Gravitational corrections in N = 1 and N = 2 supersymmetric gauge theories are obtained from topological string amplitudes. We show how they are recovered in matrix model computations. This provides a test of the proposal by Dijkgraaf and Vafa beyond the planar limit. Both, matrix model and topological string theory, are used to check a conjecture of Nekrasov concerning these gravitational couplings in Seiberg-Witten theory. Our analysis is performed for those gauge theories which are related to the cubic matrix model, i.e. pure SU(2) Seiberg-Witten theory and N = 2 U(N) SYM broken to N = 1 via a cubic superpotential. We outline the computation of the topological amplitudes for the local Calabi-Yau manifolds which are relevant for these two cases.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/3557122221b2996021d021d53055b5423a9cd99c
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Citations in the corpus
- Quantum geometry of refined topological strings (2011, unknown): “, [64]) ∆1 = z1z2 , ∆2 = √ δ2 − 2(z1 + z2) , ∆3 = (δ(2) − 3z1)(2) − 6z2δ(2) + 9z(2) 2 + 14z1z2 , where κI(β) are β-dependent coefficients.”
- Gravity Induced C-Deformation (2003, unknown): “This prediction has already been tested in a number of cases: for the gravitational correction for N = 4 Yang-Mills in the third paper in [1], and for certain N = 2 supersymmetric gauge systems in [10,11].”
- Holomorphic anomaly in gauge theories and matrix models (2006, methodology): “Also at one loop the conjecture holds(6) [8, 10].”
- From Weak to Strong Coupling in ABJM Theory (2010, unknown): “These expressions differ from the ones in [66] in a permutation of the roots, as explained in [67].”
- Supersymmetric Gauge Theories, Intersecting Branes and Free Fermions (2007, background): “Including all string loop corrections the free fermion theory is elegantly formulated in terms of holonomic D-modules that replace the classical holomorphic curve in the quantum case.”
- Nonperturbative effects and nonperturbative definitions in matrix models and topological strings (2008, background): “6.1 General picture 41 6.2 A toy model 42 6.3 Holographic description and nonperturbative effects 44”
- Topological Strings and (Almost) Modular Forms (2006, methodology): “can be rewritten, using the results we have obtained so far, as [26]”
- Instanton Counting and Chern-Simons Theory (2002, background): “For the N = 2 D=4 SU(2) theory this has been confirmed by comparing the results from the topologically twisted theory and matrix model calculations [19, 27].”
- Hermitian matrix model free energy: Feynman graph technique for all genera (2005, unknown): “We consider solutions to the loop equations admitting multi-matrix integral representations [6, 12, 13].”
- Topological strings and Nekrasov's formulas (2003, result): “We have computed P (k) g for F0 and found a precise agreement with the results reported in [ 28 , 21]”
- Les Houches lectures on matrix models and topological strings (2004, methodology): “One finds, up to fourth order in the coupling constant β, the following result [45]:”