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The gauge structure of the four dimensional effective theory (4DET) arising from a pure Yang-Mills theory in five dimensions compactified on the orbifold $S^1/Z_2$ is reexamined on the basis of the BRST symmetry. The two scenarios that can…

高能物理 - 唯象学 · 物理学 2011-01-18 H. Novales-Sánchez , J. J. Toscano

We start from a pure Yang-Mills theory defined on a spacetime with one universal extra dimension that we orbifold-compactify. We obtain a Kaluza-Klein (KK) theory by expanding in KK towers covariant objects rather than fields, as such an…

高能物理 - 唯象学 · 物理学 2012-06-21 H. Novales-Sánchez

A five dimensional pure Yang--Mills theory, with the fifth coordinate compactified on the orbifold $S^1/Z_2$ of radius R, leads to a four dimensional theory which is governed by two types of local gauge transformations, namely, the well…

高能物理 - 唯象学 · 物理学 2011-11-17 H. Novales-Sánchez , J. J. Toscano

Effects of universal extra dimensions on Standard Model observables first arise at the one-loop level. The quantization of this class of theories is therefore essential in order to perform predictions. A comprehensive study of the Standard…

高能物理 - 唯象学 · 物理学 2012-04-24 A. Cordero-Cid , M. Gómez-Bock , H. Novales-Sánchez , J. J. Toscano

Gauge theories formulated in a space-time manifold that includes compact extra dimensions can show a nontrivial gauge structure. Depending on whether the gauge parameters propagate or not in the extra dimensions, two different Kaluza--Klein…

高能物理 - 唯象学 · 物理学 2015-05-28 H. Novales-Sánchez , J. J. Toscano

The one-loop contribution of the excited Kaluza-Klein (KK) modes of the $SU_L(2)$ gauge group on the off-shell $WW\gamma$ and $WWZ$ vertices is calculated in the context of a pure Yang-Mills theory in five dimensions and its…

高能物理 - 唯象学 · 物理学 2011-02-16 A. Flores-Tlalpa , J. Montano , H. Novales-Sánchez , F. Ramirez-Zavaleta , J. J. Toscano

In this article we study Kaluza-Klein (KK) dimensional reduction of massive Abelian gauge theories with charged matter fields on a circle. Since local gauge transformations change position dependence of the charged fields, the decomposition…

高能物理 - 理论 · 物理学 2016-07-11 Kazuyuki Furuuchi

The radiative correction to beta function is comprehensively studied at 1 loop in the context of universal extra dimensions. Instead of using cutoffs to regularize 1-loop divergences, the dimensional regularization scheme is used. Large…

高能物理 - 唯象学 · 物理学 2020-07-01 M. Huerta-Leal , H. Novales-Sánchez , J. J. Toscano

In this paper we examine the 4-dimensional effective theory for the light Kaluza-Klein (KK) modes. Our main interest is in the interaction terms. We point out that the contribution of the heavy KK modes is generally needed in order to…

高能物理 - 理论 · 物理学 2008-11-26 S. Randjbar-Daemi , A. Salvio , M. Shaposhnikov

The well-known Yang-Mills theory with one $ S^{1} / Z_{2}$ universal extra dimension (UED) is generalized to an arbitrary number of spatial extra dimensions through a novel compactification scheme. In this paper, the Riemannian flat based…

高能物理 - 理论 · 物理学 2015-02-04 M. A. López-Osorio , E. Martínez-Pascual , H. Novales-Sánchez , J. J. Toscano

We construct gauge theories in two extra dimensions compactified on the chiral square, which is a simple compactification that leads to chiral fermions in four dimensions. Stationarity of the action on the boundary specifies the boundary…

高能物理 - 唯象学 · 物理学 2009-11-11 Gustavo Burdman , Bogdan A. Dobrescu , Eduardo Ponton

We study in detail the issue of gauge-fixing in theories with one universal extra dimension, i.e. theories where both bosons and fermions display Kaluza-Klein (KK) excitations. The extra dimension is compactified using the standard orbifold…

高能物理 - 唯象学 · 物理学 2009-11-07 Joannis Papavassiliou , Arcadi Santamaria

We consider the 4D effective theory for the light Kaluza-Klein (KK) modes. The heavy KK mode contribution is generally needed to reproduce the correct physical predictions: an equivalence, between the effective theory and the D-dimensional…

高能物理 - 理论 · 物理学 2008-11-26 A. Salvio

We construct a manifestly gauge invariant Lagrangian in 3+1 dimensions for N Kaluza-Klein modes of an SU(m) gauge theory in the bulk. For example, if the bulk is 4+1, the effective theory is \Pi_{i=1}^{N+1} SU(m)_i with N chiral (\bar{m},m)…

高能物理 - 理论 · 物理学 2009-11-07 Christopher T. Hill , Stefan Pokorski , Jing Wang

We provide an explicit construction of a manifestly duality invariant, interacting deformation of Maxwell theory in four dimensions in terms of mutually local, but interacting 1- and 3-forms. Interestingly, our theory is formulated directly…

高能物理 - 理论 · 物理学 2026-01-12 Carlo Alberto Cremonini , Erik Hundeshagen , Ivo Sachs

The Euclidean version of the Yang-Mills theory is studied in four dimensions. The field is expressed non-linearly in terms of the basic variables. The field is developed inductively, adding one excitation at a time. A given excitation is…

高能物理 - 唯象学 · 物理学 2016-09-01 Paul Federbush

We deepen the understanding of the quantization of the Yang-Mills field by showing that the concept of gauge fixing in 4 dimensions is replaced in the 5-dimensional formulation by a procedure that amounts to an $A$-dependent gauge…

高能物理 - 理论 · 物理学 2016-09-06 Laurent Baulieu , Daniel Zwanziger

We study five-dimensional Yang-Mills theories compactified on an S^1/Z_2 orbifold. The fundamental Lagrangian naturally includes brane kinetic terms at the orbifold fixed points which are induced by quantum corrections of the bulk fields.…

高能物理 - 唯象学 · 物理学 2007-05-23 L. Nilse

We study quantized Yang-Mills theory with massive vector fields in the framework of causal perturbation theory. The most general form of the interaction which is invariant under operator gauge transformations is pointed out. The generator…

高能物理 - 理论 · 物理学 2007-05-23 Frank Krahe

We perform a Kaluza-Klein inspired rewriting of double field theory by splitting the coordinates into `compact' and `non-compact' directions. There is no truncation of the compact coordinates or their duals, and so this formulation is…

高能物理 - 理论 · 物理学 2013-10-30 Olaf Hohm , Henning Samtleben
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