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Related papers: Charge sum rules in N=2 theories

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We prove that N=2 theories that arise by taking n free hypermultiplets and gauging a subgroup of Sp(n), the non-R global symmetry of the free theory, have a remaining global symmetry which is a direct sum of unitary, symplectic, and special…

High Energy Physics - Theory · Physics 2013-12-13 Jock McOrist , Ilarion V. Melnikov , Brian Wecht

The importance of the nonlinear corrections on the momentum sum rule is investigated on the initial scale $Q_{0}^2$. Nonlinear corrections are found to play an indispensable role in the singlet and gluon momentum sum rule in the high-order…

High Energy Physics - Phenomenology · Physics 2024-08-20 G. R. Boroun

Recently, a longitudinal sum rule for the electric polarizability of nuclei was used to revise a relativistic correction in a dipole sum rule for the polarizability (nucl-th/9802011). This revision is shown to be wrong because of neglecting…

Nuclear Theory · Physics 2009-10-31 A. I. L'vov

Anomalous dimension and higher conserved charges in the $sl(2)$ sector of ${\cal N}=4$ SYM for generic spin $s$ and twist $L$ are described by using a novel kind of non-linear integral equation (NLIE). The latter can be derived under…

High Energy Physics - Theory · Physics 2009-02-02 Diego Bombardelli , Davide Fioravanti , Marco Rossi

Contents: 1. Introduction. 2. Sum rules prior to QCD. 3. Dispersion relations. 4. Types of two point function sum rules. 5. Non-perturbative power corrections. 6. Some examples of QCD sum rules.

High Energy Physics - Phenomenology · Physics 2016-09-06 Eduardo de Rafael

It is shown that N=2 supersymmetric theories with central charges present some hidden quartic symmetry. This enables us to construct representations of the quartic structure induced by superalgebra representations.

High Energy Physics - Theory · Physics 2014-11-21 R. Campoamor-Stursberg , M. Rausch de Traubenberg

A general class of inverse-moment sum rules was previously derived by the authors in a chiral perturbation theory (ChPT) study at two-loop order of the isospin and hypercharge vector-current propagators. Here, we address the evaluation of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eugene Golowich , Joachim Kambor

We study non-planar corrections in two special $\mathcal N=2$ superconformal $SU(N)$ gauge theories that are planar-equivalent to $\mathcal N=4$ SYM theory: two-nodes quiver model with equal couplings and $\mathcal N=2$ vector multiplet…

High Energy Physics - Theory · Physics 2023-06-07 M. Beccaria , G. P. Korchemsky , A. A. Tseytlin

This version of the paper corrects an inaccuracy in the proof of Theorem 2.9 in the published version. The main results remain unchanged.

Number Theory · Mathematics 2023-01-02 Florin P. Boca , Alexandru Zaharescu

We show that previous correspondence between some (integrable) statistical field theory quantities and periods of $SU(2)$ $\mathcal{N}=2$ deformed gauge theory still holds if we add $N_f=1,2$ flavours of matter. Moreover, the correspondence…

High Energy Physics - Theory · Physics 2025-10-07 Davide Fioravanti , Daniele Gregori , Hongfei Shu

We study the conformal invariance of non-planar beta-deformed N=4 SYM theory using the coupling constant reduction (CCR) formalism. We show that up to order g^10, differently from the planar case, we can remove the scheme dependence in the…

High Energy Physics - Theory · Physics 2007-10-26 Federico Elmetti , Andrea Mauri , Marco Pirrone

We show that N=1/2 supersymmetric gauge theory is renormalisable at one loop, but only after gauge invariance is restored in a non-trivial fashion.

High Energy Physics - Theory · Physics 2009-11-10 I. Jack , D. R. T. Jones , L. A. Worthy

A noncommutative version of the usual electro-weak theory is constructed. We discuss how to overcome the two major problems: 1) although we can have noncommutative U(n) (which we denote by $U_{\star}(n)$) gauge theory we cannot have…

High Energy Physics - Theory · Physics 2010-05-28 M. Chaichian , P. Presnajder , M. M. Sheikh-Jabbari , A. Tureanu

We define the notion of a complete N=2 supersymmetric theory in 4 dimensions as a UV complete theory for which all the BPS central charges can be arbitrarily varied as we vary its Coulomb branch parameters, masses, and coupling constants.…

High Energy Physics - Theory · Physics 2013-04-12 Sergio Cecotti , Cumrun Vafa

We present the next-to-next-to-leading order ($\alpha \alpha_s^2$) corrections to the first moment of the polarized virtual photon structure function $g_1^\gamma(x,Q^2,P^2)$ in the kinematical region $Q^2\gg P^2 \gg \Lambda^2$ in QCD. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Ueda , T. Uematsu , K. Sasaki

A class of exact non-renormalized extremal correlators of half-BPS operators in N=4 SYM, with U(N) gauge group, is shown to satisfy finite factorization equations reminiscent of topological gauge theories. The finite factorization equations…

High Energy Physics - Theory · Physics 2009-11-07 Steven Corley , Sanjaye Ramgoolam

(One typo corrected and one incorrect statement removed. Extra details on conserved quantities and symmetry algebras added).

General Relativity and Quantum Cosmology · Physics 2009-10-22 James D. E. Grant

We investigate 2d $\mathcal{N}=(0,4)$ supersymmetric theories obtained from a topologically-twisted reduction of 4d $\mathcal{N}=2$ class $\mathcal{S}$ theories on a Riemann surface. This study addresses subtle aspects of central charges,…

High Energy Physics - Theory · Physics 2026-05-25 Wei Cui , Junkang Huang , Zi-Xiao Huang , Satoshi Nawata , Shutong Zhuang

For $n \ge 2$, Gamburd, Jakobson, and Sarnak [J. Eur. Math. Soc. 1, 51-85 (1999)] conjectured that almost every $n$-tuple in $\mathrm{SU}(2)$ has a spectral gap. Toward this conjecture, Fisher [Int. Math. Res. Not. (2006)] established a…

Group Theory · Mathematics 2026-03-19 Oleg Pikhurko , Kohki Sakamoto

We compare the mass spectra and string tensions of SU(2), SU(3) and SU(4) gauge theories in 2+1 dimensions. We find that the ratios of masses are, to a first approximation, independent of N and that the remaining dependence can be…

High Energy Physics - Lattice · Physics 2009-10-30 M. Teper