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Related papers: Two-dimensional QCD and instanton contribution

200 papers

We show that every gravitational instantons are SU(2) Yang-Mills instantons on a Ricci-flat four manifold although the reverse is not necessarily true. It is shown that gravitational instantons satisfy exactly the same self-duality equation…

High Energy Physics - Theory · Physics 2011-04-28 John J. Oh , Chanyong Park , Hyun Seok Yang

We show how to formulate Yang-Mills Theory in \m{2+1} dimensions as a hamitonian system within a simplicial regularization and construct its quantization, with special attention to the mass gap. An approximate conformal invariance of the…

High Energy Physics - Theory · Physics 2017-08-23 S. G. Rajeev

QCD point-to-point correlation functions at distances .2-1 fm are very different for different channels, and they tell us a lot about inter-quark interactions. Recent studies based on experimental data, 'instanton liquid' approach and…

High Energy Physics - Lattice · Physics 2009-10-22 E. Shuryak

We discuss the reality properties of the fermionic collective coordinates in Euclidean space in an instanton background and construct hermitean actions for N = 4 and N = 2 supersymmetric Euclidean Yang-Mills theories.

High Energy Physics - Theory · Physics 2009-10-31 A. V. Belitsky , S. Vandoren , P. van Nieuwenhuizen

We study the quark confinement problem in 2+1 dimensional pure Yang-Mills theory using euclidean instanton methods. The instantons are regularized and dressed Wu-Yang monopoles. The dressing of a monopole is due to the mean field of the…

High Energy Physics - Theory · Physics 2009-10-28 Sumit R. Das , Spenta R. Wadia

We apply equivariant integration technique, developed in the context of instanton counting, to two dimensional N=2 supersymmetric Yang-Mills models. Twisted superpotential for U(N) model is computed. Connections to the four dimensional case…

High Energy Physics - Theory · Physics 2010-10-27 Sergey Shadchin

Our goal is to discover possible new 4-dimensional euclidean solutions (instantons) in fundamental SU(2) Yang-Mills-Higgs theory, with a constraint added to prevent collapse of the scale. We show that, most likely, there exists one…

High Energy Physics - Phenomenology · Physics 2009-10-22 F. R. Klinkhamer

We consider instanton contributions to chiral correlators, such as <0| Tr \lambda^2 (x) Tr \lambda^2(x') |0>, in N=1 supersymmetric Yang-Mills theory with either light adjoint or fundamental matter. Within the former model, extraction of…

High Energy Physics - Theory · Physics 2015-06-26 Adam Ritz , Arkady Vainshtein

I develop a formalism for solving topological field theories explicitly, in the case when the explicit expression of the instantons is known. I solve topological Yang-Mills theory with the $k=1$ Belavin {\sl et al.} instanton and…

High Energy Physics - Theory · Physics 2009-10-28 Damiano Anselmi

The SL(2,C) Yang-Mills instanton solutions constructed recently by the biquaternion method were shown to satisfy the complex version of the ADHM equations and the Monad construction. Moreover, we discover that, in addition to the…

High Energy Physics - Theory · Physics 2018-03-14 Sheng-Hong Lai , Jen-Chi Lee , I-Hsun Tsai

We pursue the intriguing possibility that larger-size instantons build up diffractive scattering, with the marked instanton-size scale $<\rho> \approx 0.5$ fm being reflected in the conspicuous ``geometrization'' of soft QCD. As an explicit…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Schrempp , A. Utermann

The n-instanton contribution to the Seiberg-Witten prepotential of N=2 supersymmetric d=4 Yang Mills theory is represented as the integral of the exponential of an equivariantly exact form. Integrating out an overall scale and a U(1) angle…

High Energy Physics - Theory · Physics 2009-11-07 R. Flume , R. Poghossian , H. Storch

We consider the $SU(N)$ Yang-Mills theory, whose topological sectors are restricted to the instanton number with integer multiples of $p$. We can formulate such a quantum field theory maintaining locality and unitarity, and the model…

High Energy Physics - Theory · Physics 2020-03-25 Yuya Tanizaki , Mithat Ünsal

The boundstate problem in 2+1-dimensional large-N Yang-Mills theory is accurately solved using the light-front Hamiltonian of transverse lattice gauge theory. We conduct a thorough investigation of the space of couplings on coarse lattices,…

High Energy Physics - Lattice · Physics 2009-10-31 S. Dalley , B. van de Sande

We investigate finite energy solutions of Yang-Mills--Chern-Simons systems in odd spacetime dimensions, d=2n+1, with n>2. This can be carried out systematically for all n, but the cases n=3,4 corresponding to a 7,8 dimensional spacetime are…

High Energy Physics - Theory · Physics 2015-06-04 Eugen Radu , D. H. Tchrakian

We review the physics of topological objects in QCD. Topics include: solitons, vortices, magnetic monopoles, instantons, (effective theories of) confinement.

High Energy Physics - Theory · Physics 2007-05-23 Gerard 't Hooft , Falk Bruckmann

The $1/N$ expansion of the weak coupling phase of two-dimensional QCD on a sphere is constructed. It is demonstrated that the phase transition from the weak to the strong coupling phase is induced by instantons. A double scaling limit of…

High Energy Physics - Theory · Physics 2009-10-28 David J. Gross , Andrei Matytsin

Three introductory lectures: on Yangians and their representations; on Yangian symmetry in 1+1D integrable (bulk) field theory; and on the effect of a boundary upon this symmetry.

High Energy Physics - Theory · Physics 2009-11-10 N. J. Mackay

I describe how integrable quantum field theories in 2 spacetime dimensions are characterized by infinite dimensional quantum group symmetries, namely the q-deformations of affine Lie algebras, and their Yangian limit. These symmetries can…

High Energy Physics - Theory · Physics 2007-05-23 Andre LeClair

We consider the self-dual Yang-Mills equations in seven dimensions. Modifying the t'Hooft construction of instantons in $d=4$, we find $N$-instanton $7d$ solutions which depend on $8N$ effective parameters and are $E_{6}$-invariant.

High Energy Physics - Theory · Physics 2009-11-11 E. K. Loginov