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To set the stage, I discuss the $\beta$-function of the massless O(N) model in three dimensions, which can be calculated exactly in the large N limit. Then, I consider SU(N) Yang-Mills theory in 2+1 space-time dimensions. Relating the…

High Energy Physics - Lattice · Physics 2021-05-19 Paul Romatschke

Using a gauge invariant exact renormalization group, we show how to compute the effective action, and extract the physics, whilst manifestly preserving gauge invariance at each and every step. As an example we give an elegant computation of…

High Energy Physics - Theory · Physics 2007-05-23 Stefano Arnone , Antonio Gatti , Tim R. Morris

We investigate N=1 super Yang-Mills theory using fractional branes. We first define the beta-function with respect to a supergravity coordinate. To provide the relation between the supergravity parameter and the renormalization group scale…

High Energy Physics - Theory · Physics 2010-04-05 Raffaele Marotta , Francesco Sannino

Working in a Hamiltonian formulation with $A_0 = 0$ gauge and also in a path integral formulation, we show that the vacuum wave functional of four-dimensional pure Yang-Mills theory has the form of the exponential of a {\it…

High Energy Physics - Theory · Physics 2009-10-30 Miyuki Kawamura , Kayoko Maeda , Makoto Sakamoto

We obtain the correct all-loop beta-function of pure N=1 super Yang-Mills theory from the supergravity solution of the warped deformed conifold, including also some nonperturbative corrections. The crucial ingredient is the gauge-gravity…

High Energy Physics - Theory · Physics 2010-04-05 Emiliano Imeroni

An algebraic criterion for the vanishing of the beta function for renormalizable quantum field theories is presented. Use is made of the descent equations following from the Wess-Zumino consistency condition. In some cases, these equations…

High Energy Physics - Theory · Physics 2008-11-26 V. E. R. Lemes , M. S. Sarandy , S. P. Sorella , O. S. Ventura , L. C. Q. Vilar

The semi-analytical $O(\alpha_s^4)$ expression for the renormalization group $\beta$-function in the ${\rm{V}}$-scheme is obtained in the case of the $SU(N_c)$ gauge group. In the process of calculations we use the existing information…

High Energy Physics - Phenomenology · Physics 2015-10-13 A. L. Kataev , V. S. Molokoedov

The partition function of four dimensional Euclidean, non-supersymmetric SU(2) Yang--Mills theory is calculated in the perturbative and weak coupling regime i.e. in a small open ball about the flat connection (what we call the vicinity of…

High Energy Physics - Theory · Physics 2023-04-11 Gabor Etesi

We study the Renormalization Group (RG) flow of critical bosonic background fields in the framework of the RG approach to string theory. In this approach quantum field theory beta-functions are the extra inputs in solving the string theory…

High Energy Physics - Theory · Physics 2009-10-31 Ian I. Kogan , Martin Schvellinger , Bayram Tekin

We perform a variational calculation in the SU(N) Yang Mills theory in 3+1 dimensions. Our trial variational states are explicitly gauge invariant, and reduce to simple Gaussian states in the zero coupling limit. Our main result is that the…

High Energy Physics - Theory · Physics 2009-10-28 Ian I. Kogan , Alex Kovner

It is proposed to use the pinch technique (PT) to obtain the gauge-independent thermal $\beta$ function in a hot Yang-Mills gas. Calculations of the thermal $\beta$ function are performed at one-loop level in four different gauges, (i) the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Ken Sasaki

We describe a nonperturbative method for calculating the QCD vacuum and glueball wave functions, based on an eigenvalue equation approach to Hamiltonian lattice gauge theory. Therefore, one can obtain more physical information than the…

High Energy Physics - Lattice · Physics 2009-10-30 J. Liu , X. Q. Luo , X. Fang , S. Guo , H. Kroeger , D. Schuette , L. Lin

We show that U(1) Yang-Mills theory on noncommutative R^4 can be renormalized at the one-loop level by multiplicative dimensional renormalization of the coupling constant and fields of the theory. We compute the beta function of the theory…

High Energy Physics - Theory · Physics 2009-10-31 C. P. Martin , D. Sanchez-Ruiz

We compute the $\beta$-function of a YM theory, broken to $U(1)$, by evaluating the coupling constant renormalization in the broken phase. We perform the calculation in the unitary gauge where only physical particles appear and the theory…

High Energy Physics - Theory · Physics 2016-09-06 G. Bimonte , R. Iengo , G. Lozano

We propose an all orders beta function for ordinary Yang-Mills theories with or without fermions inspired by the Novikov-Shifman-Vainshtein-Zakharov beta function of N=1 supersymmetric gauge theories. The beta function allows us to bound…

High Energy Physics - Theory · Physics 2008-11-07 Thomas A. Ryttov , Francesco Sannino

We split the Yang-Mills Lagrangian into a free and an interaction part in such a way, that the free part is non-local and contains an arbitrary form factor. Manifest gauge invariance is guaranteed by connecting the field-strength tensors at…

High Energy Physics - Phenomenology · Physics 2016-09-06 Dieter Gromes

QED based on $\theta$-unexpanded noncomutative space-time in contrast with the noncommutative QED based on $\theta$-expanded U(1) gauge theory via the Seiberg-Witten map, is one-loop renormalizable. Meanwhile it suffers from asymptotic…

High Energy Physics - Phenomenology · Physics 2015-05-20 M. M. Ettefaghi , M. Haghighat , R. Mohammadi

We investigate -- as an alternative to usual Monte Carlo Renormalization Group methods -- the feasibility of extracting QCD beta-functions directly from a lattice analysis of correlations between the action and Wilson loops. We test this…

High Energy Physics - Lattice · Physics 2009-10-28 G. S. Bali , Ch. Schlichter , K. Schilling

The quantum Yang-Mills theory, describing a system of fields with non-dual (chromo-electric g) and dual (chromo-magnetic \tilde g) charges and revealing the generalized dual symmetry, is developed by analogy with the Zwanziger formalism in…

High Energy Physics - Phenomenology · Physics 2010-05-27 C. R. Das , L. V. Laperashvili , H. B. Nielsen

The manifestly gauge invariant Exact Renormalisation Group provides a framework for performing continuum computations in SU(N) Yang-Mills theory, without fixing the gauge. We use this formalism to compute the two-loop beta function in a…

High Energy Physics - Theory · Physics 2009-11-11 Tim R. Morris , Oliver J. Rosten