5,262 research outputs found

    Superconformal indices of three-dimensional theories related by mirror symmetry

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    Recently, Kim and Imamura and Yokoyama derived an exact formula for superconformal indices in three-dimensional field theories. Using their results, we prove analytically the equality of superconformal indices in some U(1)-gauge group theories related by the mirror symmetry. The proofs are based on the well known identities of the theory of qq-special functions. We also suggest the general index formula taking into account the U(1)JU(1)_J global symmetry present for abelian theories.Comment: 17 pages; minor change

    Discrete Darboux transformation for discrete polynomials of hypergeometric type

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    Darboux Transformation, well known in second order differential operator theory, is applied here to the difference equation satisfied by the discrete hypergeometric polynomials(Charlier, Meixner-Krawchuk, Hahn)

    Reconstruction of dielectric constants of multi-layered optical fibers using propagation constants measurements

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    We present new method for the numerical reconstruction of the variable refractive index of multi-layered circular weakly guiding dielectric waveguides using the measurements of the propagation constants of their eigenwaves. Our numerical examples show stable reconstruction of the dielectric permittivity function ε\varepsilon for random noise level using these measurements

    On the structure of the top homology group of the Johnson kernel

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    The Johnson kernel is the subgroup Kg\mathcal{K}_g of the mapping class group Mod(Σg){\rm Mod}(\Sigma_{g}) of a genus gg oriented closed surface Σg\Sigma_{g} generated by all Dehn twists about separating curves. In this paper we study the structure of the top homology group H2g3(Kg,Z){\rm H}_{2g-3}(\mathcal{K}_g, \mathbb{Z}). For any collection of 2g32g-3 disjoint separating curves on Σg\Sigma_{g} one can construct the corresponding abelian cycle in the group H2g3(Kg,Z){\rm H}_{2g-3}(\mathcal{K}_g, \mathbb{Z}); such abelian cycles will be called simplest. In this paper we describe the structure of Z[Mod(Σg)/Kg]\mathbb{Z}[{\rm Mod}(\Sigma_{g})/ \mathcal{K}_g]-module on the subgroup of H2g3(Kg,Z){\rm H}_{2g-3}(\mathcal{K}_g, \mathbb{Z}) generated by all simplest abelian cycles and find all relations between them.Comment: 22 page

    The top homology group of the genus 3 Torelli group

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    The Torelli group of a genus gg oriented surface Σg\Sigma_g is the subgroup Ig\mathcal{I}_g of the mapping class group Mod(Σg){\rm Mod}(\Sigma_g) consisting of all mapping classes that act trivially on H1(Σg,Z){\rm H}_1(\Sigma_g, \mathbb{Z}). The quotient group Mod(Σg)/Ig{\rm Mod}(\Sigma_g) / \mathcal{I}_g is isomorphic to the symplectic group Sp(2g,Z){\rm Sp}(2g, \mathbb{Z}). The cohomological dimension of the group Ig\mathcal{I}_g equals to 3g53g-5. The main goal of the present paper is to compute the top homology group of the Torelli group in the case g=3g = 3 as Sp(6,Z){\rm Sp}(6, \mathbb{Z})-module. We prove an isomorphism H4(I3,Z)IndS3SL(2,Z)×3Sp(6,Z)Z,{\rm H}_4(\mathcal{I}_3, \mathbb{Z}) \cong {\rm Ind}^{{\rm Sp}(6, \mathbb{Z})}_{S_3 \ltimes {\rm SL}(2, \mathbb{Z})^{\times 3}} \mathcal{Z}, where Z\mathcal{Z} is the quotient of Z3\mathbb{Z}^3 by its diagonal subgroup Z\mathbb{Z} with the natural action of the permutation group S3S_3 (the action of SL(2,Z)×3{\rm SL}(2, \mathbb{Z})^{\times 3} is trivial). We also construct an explicit set of generators and relations for the group H4(I3,Z){\rm H}_4(\mathcal{I}_3, \mathbb{Z}).Comment: 35 pages, minor correction

    On a modular property of N=2 superconformal theories in four dimensions

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    In this note we discuss several properties of the Schur index of N=2 superconformal theories in four dimensions. In particular, we study modular properties of this index under SL(2,Z) transformations of its parameters.Comment: 23 page, 2 figure

    Driving Operators Relevant: A Feature of Chern-Simons Interaction

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    By computing anomalous dimensions of gauge invariant composite operators (ψˉψ)n(\bar\psi\psi)^n and (ϕϕ)n(\phi^*\phi)^n in Chern-Simons fermion and boson models, we address that Chern-Simons interactions make these operators more relevant or less irrelevant in the low energy region. We obtain a critical Chern-Simons fermion coupling, 1κc2=619{1\over \kappa_c^2} = {6\over 19}, for a phase transition at which the leading irrelevant four-fermion operator (ψˉψ)2(\bar\psi\psi)^2 becomes marginal, and a critical Chern-Simons boson coupling, 1κc2=634{1\over \kappa_c^2} = {6\over 34}, for a similar phase transition for the leading irrelevant operator (ϕϕ)4(\phi^*\phi)^4. We see this phenomenon also in the 1/N1/N expansion.Comment: (ten pages, latex, figures included

    Self-Similar Potentials and the q-Oscillator Algebra at Roots of Unity

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    Properties of the simplest class of self-similar potentials are analyzed. Wave functions of the corresponding Schr\"odinger equation provide bases of representations of the qq-deformed Heisenberg-Weyl algebra. When the parameter qq is a root of unity the functional form of the potentials can be found explicitly. The general q3=1q^3=1 and the particular q4=1q^4=1 potentials are given by the equianharmonic and (pseudo)lemniscatic Weierstrass functions respectively.Comment: 15 pp, Latex, to appear in Lett.Math.Phy

    S-duality and 2d Topological QFT

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    We study the superconformal index for the class of N=2 4d superconformal field theories recently introduced by Gaiotto. These theories are defined by compactifying the (2,0) 6d theory on a Riemann surface with punctures. We interpret the index of the 4d theory associated to an n-punctured Riemann surface as the n-point correlation function of a 2d topological QFT living on the surface. Invariance of the index under generalized S-duality transformations (the mapping class group of the Riemann surface) translates into associativity of the operator algebra of the 2d TQFT. In the A_1 case, for which the 4d SCFTs have a Lagrangian realization, the structure constants and metric of the 2d TQFT can be calculated explicitly in terms of elliptic gamma functions. Associativity then holds thanks to a remarkable symmetry of an elliptic hypergeometric beta integral, proved very recently by van de Bult.Comment: 25 pages, 11 figure
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