811 research outputs found

    Wilson Loops and Chiral Correlators on Squashed Sphere

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    We study chiral deformations of N=2{\cal N}=2 and N=4{\cal N}=4 supersymmetric gauge theories obtained by turning on τJ tr ΦJ\tau_J \,{\rm tr} \, \Phi^J interactions with Φ\Phi the N=2{\cal N}=2 superfield. Using localization, we compute the deformed gauge theory partition function Z(τ⃗∣q)Z(\vec\tau|q) and the expectation value of circular Wilson loops WW on a squashed four-sphere. In the case of the deformed N=4{\cal N}=4 theory, exact formulas for ZZ and WW are derived in terms of an underlying U(N)U(N) interacting matrix model replacing the free Gaussian model describing the N=4{\cal N}=4 theory. Using the AGT correspondence, the τJ\tau_J-deformations are related to the insertions of commuting integrals of motion in the four-point CFT correlator and chiral correlators are expressed as τ\tau-derivatives of the gauge theory partition function on a finite Ω\Omega-background. In the so called Nekrasov-Shatashvili limit, the entire ring of chiral relations is extracted from the ϵ\epsilon-deformed Seiberg-Witten curve. As a byproduct of our analysis we show that SU(2)SU(2) gauge theories on rational Ω\Omega-backgrounds are dual to CFT minimal models.Comment: 33 pages, 2 figure, in this version we have added two new references and a detailed comparison with the results obtained in one of these tw

    Exotic prepotentials from D(-1)D7 dynamics

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    We compute the partition functions of D(-1)D7 systems describing the multi-instanton dynamics of SO(N) gauge theories in eight dimensions. This is the simplest instance of the so called exotic instantons. In analogy with the Seiberg-Witten theory in four space-time dimensions, the prepotential and correlators in the chiral ring are derived via localization formulas and found to satisfy relations of the Matone type. Exotic prepotentials of SO(N) gauge theories with N=2 supersymmetries in four-dimensions are also discussed.Comment: 19 page

    Structure Constants in the N=1N=1 Super-Liouville Field Theory

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    The symmetry algebra of N=1N=1 Super-Liouville field theory in two dimensions is the infinite dimensional N=1N=1 superconformal algebra, which allows one to prove, that correlation functions, containing degenerated fields obey some partial linear differential equations. In the special case of four point function, including a primary field degenerated at the first level, this differential equations can be solved via hypergeometric functions. Taking into account mutual locality properties of fields and investigating s- and t- channel singularities we obtain some functional relations for three- point correlation functions. Solving this functional equations we obtain three-point functions in both Neveu-Schwarz and Ramond sectors.Comment: LaTeX file, 17 pages, no figure

    Perturbation theory in radial quantization approach and the expectation values of exponential fields in sine-Gordon model

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    A perturbation theory for Massive Thirring Model (MTM) in radial quantization approach is developed. Investigation of the twisted sector in this theory allows us to calculate the vacuum expectation values of exponential fields expiaphi(0) exp iaphi (0) of the sine-Gordon theory in first order over Massive Thirring Models coupling constant. It appears that the apparent difficulty in radial quantization of massive theories, namely the explicite ''time'' dependence of the Hamiltonian, may be successfully overcome. The result we have obtained agrees with the exact formula conjectured by Lukyanov and Zamolodchikov and coincides with the analogous calculations recently carried out in dual angular quantization approach by one of the authors.Comment: 16 pages, no figures, LaTe
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