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Related papers: \beta-deformed matrix model and Nekrasov partition…

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We study \beta-deformed matrix models with Penner type potentials, which correspond to N=2 SU(2) supersymmetric gauge theories with N_F=2,3, and 4 flavors. We compute explicitly the genus one corrections to the free energy of the matrix…

High Energy Physics - Theory · Physics 2013-05-06 Jong-Hyun Baek

We consider the half-genus expansion of the resolvent function in the $\beta$-deformed matrix model with three-Penner potential under the AGT conjecture and the $0d-4d$ dictionary. The partition function of the model, after the…

High Energy Physics - Theory · Physics 2011-11-28 Hiroshi Itoyama , Nobuhiro Yonezawa

We relate Nekrasov partition functions, with arbitrary values of $\epsilon_1,\epsilon_2$ parameters, to matrix models for $\beta$-ensembles. We find matrix models encoding the instanton part of Nekrasov partition functions, whose measure,…

High Energy Physics - Theory · Physics 2010-04-30 Piotr Sułkowski

We observe that, at beta-deformed matrix models for the four-point conformal block, the point q=0 is the point where the three-Penner type model becomes a pair of decoupled two-Penner type models and where, in the planar limit, (an array…

High Energy Physics - Theory · Physics 2014-11-20 Hiroshi Itoyama , Takeshi Oota

The relation between the Seiberg-Witten prepotentials, Nekrasov functions and matrix models is discussed. We derive quasiclassically the matrix models of Eguchi-Yang type, describing the instantonic contribution to the deformed partition…

High Energy Physics - Theory · Physics 2012-02-03 A. Marshakov

This is the fourth article in the collection of reviews "Exact results on N=2 supersymmetric gauge theories", ed. J.Teschner. It describes a very useful mathematical representation of the results of the localisation computations of…

High Energy Physics - Theory · Physics 2015-02-25 Kazunobu Maruyoshi

The Penner type beta-ensemble for Omega-deformed N=2 SU(2) gauge theory with two massless flavors arising as a limiting case from the AGT conjecture is considered. The partition function can be calculated perturbatively in a saddle-point…

High Energy Physics - Theory · Physics 2013-03-14 Daniel Krefl

The AGT conjecture relates \mathcal{N}=2 4d SUSY gauge theories to 2d CFTs. Matrix model techniques can be used to investigate both sides of this relation. The large N limit refers here to the size of Young tableaux in the expression of the…

High Energy Physics - Theory · Physics 2013-07-02 Jean-Emile Bourgine

The AGT relation identifies the Nekrasov functions for various N=2 SUSY gauge theories with the 2d conformal blocks, which possess explicit Dotsenko-Fateev matrix model (beta-ensemble) representations the latter being polylinear…

High Energy Physics - Theory · Physics 2011-03-30 A. Mironov , A. Morozov , Sh. Shakirov

In this note we present some results on the convergence of Nekrasov partition functions as power series in the instanton counting parameter. We focus on $U(N)$ ${\mathcal N}=2$ gauge theories in four dimensions with matter in the adjoint…

High Energy Physics - Theory · Physics 2023-11-30 Paolo Arnaudo , Giulio Bonelli , Alessandro Tanzini

We present an implementation of the method of orthogonal polynomials which is particularly suitable to study the partition functions of Penner random matrix models, to obtain their explicit forms in the exactly solvable cases, and to…

Mathematical Physics · Physics 2014-07-24 Gabriel Álvarez , Luis Martínez Alonso , Elena Medina

The AGT conjecture claims an equivalence of conformal blocks in 2d CFT and sums of Nekrasov functions (instantonic sums in 4d SUSY gauge theory). The conformal blocks can be presented as Dotsenko-Fateev beta-ensembles, hence, the AGT…

High Energy Physics - Theory · Physics 2011-03-18 A. Mironov , A. Morozov , Sh. Shakirov

We derive an infinite set of recursion formulae for Nekrasov instanton partition function for linear quiver U(N) supersymmetric gauge theories in 4D. They have a structure of a deformed version of W_{1+\infty} algebra which is called SH^c…

High Energy Physics - Theory · Physics 2013-08-09 Shoichi Kanno , Yutaka Matsuo , Hong Zhang

A matrix model approach to proof of the AGT relation is briefly reviewed. It starts from the substitution of conformal blocks by the Dotsenko-Fateev beta-ensemble averages and Nekrasov functions by a double deformation of the exponentiated…

High Energy Physics - Theory · Physics 2012-01-05 A. Mironov , A. Morozov , Sh. Shakirov

We consider the $\Omega$-deformed $\mathcal{N}=2$ $SU(2)$ gauge theory in four dimensions with $N_{f}=4$ massive fundamental hypermultiplets. The low energy effective action depends on the deformation parameters $\varepsilon_{1},…

High Energy Physics - Theory · Physics 2017-01-04 Matteo Beccaria , Alberto Fachechi , Guido Macorini , Luigi Martina

In arXiv:0910.5670 we suggested that the Nekrasov function with one non-vanishing deformation parameter \epsilon is obtained by the standard Seiberg-Witten contour-integral construction. The only difference is that the Seiberg-Witten…

High Energy Physics - Theory · Physics 2011-07-19 A. Mironov , A. Morozov

We study the dual descriptions recently discovered for the Seiberg-Witten theory in the presence of surface operators. The Nekrasov partition function for a four-dimensional N=2 gauge theory with a surface operator is believed equal to the…

High Energy Physics - Theory · Physics 2014-11-21 Kazunobu Maruyoshi , Masato Taki

In the present work certain features of the Penner model, such its enumerative meaning and its relation to the Chern-Simons theory on the 3-sphere, are reviewed. Also, some features related to geometric transitions at the level of the…

High Energy Physics - Theory · Physics 2011-09-20 O. P. Santillan

We study the low energy effective action of the $\Omega$-deformed $\mathcal N =2^{*}$ $SU(2) $ gauge theory. It depends on the deformation parameters $\epsilon_{1},\epsilon_{2}$, the scalar field expectation value $a$, and the…

High Energy Physics - Theory · Physics 2016-08-24 Matteo Beccaria , Guido Macorini

We consider a series of massive scaling limits m_1 -> infty, q -> 0, lim m_1 q = Lambda_{3} followed by m_4 -> infty, Lambda_{3} -> 0, lim m_4 Lambda_{3} = (Lambda_2)^2 of the beta-deformed matrix model of Selberg type (N_c=2, N_f=4) which…

High Energy Physics - Theory · Physics 2010-11-11 H. Itoyama , T. Oota , N. Yonezawa
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