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We evaluate the effective actions of supersymmetric matrix models on fuzzy S^2\times S^2 up to the two loop level. Remarkably it turns out to be a consistent solution of IIB matrix model. Based on the power counting and SUSY cancellation…

High Energy Physics - Theory · Physics 2011-07-19 T. Imai , Y. Kitazawa , Y. Takayama , D. Tomino

We calculate the energy spectrum of a k=2 flux tube that is closed around a spatial torus, as a function of its length l. We do so for SU(4) and SU(5) gauge theories in 2 space dimensions. We find that to a very good approximation the…

High Energy Physics - Lattice · Physics 2009-05-12 Andreas Athenodorou , Barak Bringoltz , Michael Teper

The U(1) gauge theory on a space with Lie type noncommutativity is constructed. The construction is based on the group of translation in Fourier space, which in contrast to space itself is commutative. In analogy with lattice gauge theory,…

High Energy Physics - Theory · Physics 2023-04-18 M. Khorrami , A. H. Fatollahi , A. Shariati

We construct noncommutative U(1) gauge theory on the fuzzy sphere S^2_N as a unitary 2N x 2N matrix model. In the quantum theory the model is equivalent to a nonabelian U(N) Yang-Mills theory on a 2 dimensional lattice with 2 plaquettes.…

High Energy Physics - Theory · Physics 2008-11-26 Badis Ydri

The one-loop free energy of the four-dimensional compact QED, which is known to be equivalent to the vector Sine-Gordon model, is calculated in the strong coupling regime. In the case, when the norm of the strength tensor of the…

High Energy Physics - Theory · Physics 2007-05-23 D. V. Antonov

We investigate infinite families of 3d N=2 superconformal Chern-Simons quivers with an arbitrarily large number of gauge groups arising on M2-branes over toric CY_4's. These theories have the same matter content and superpotential of those…

High Energy Physics - Theory · Physics 2015-06-04 Antonio Amariti , Sebastian Franco

The structure of loop corrections is examined in a scalar field theory on a three dimensional space whose spatial coordinates are noncommutative and satisfy SU(2) Lie algebra. In particular, the 2- and 4-point functions in $\phi^4$ scalar…

High Energy Physics - Theory · Physics 2008-11-26 H. Komaie-Moghaddam , M. Khorrami , A. H. Fatollahi

Lattice gauge theories with gauge groups SO(3) and SU(2) are compared. The free energy of electric twist, an order parameter for the confinement-deconfinement transition which does not rely on centre-symmetry breaking, is measured in both…

High Energy Physics - Lattice · Physics 2009-11-07 Philippe de Forcrand , Oliver Jahn

We revisit an orbifold matrix model obtained as a restriction of the type IIB matrix model on a Z_3-invariant sector. An investigation of its moduli space of vacua is performed and issues related to chiral gauge theory and gravity are…

High Energy Physics - Theory · Physics 2012-05-01 Athanasios Chatzistavrakidis , Harold Steinacker , George Zoupanos

The full U-duality symmetry of toroidally compactified M-theory can only be displayed by allowing non-rectangular tori with expectation values of the gauge fields. We construct an E_d(Z) U-duality invariant mass formula incorporating…

High Energy Physics - Theory · Physics 2010-11-19 N. A. Obers , B. Pioline , E. Rabinovici

We report on the construction of four dimensional gauged supergravity models that can be interpreted as type IIB orientifold compactification in presence of 3-form fluxes and D3--branes. We mainly address our attention to the symplectic…

High Energy Physics - Theory · Physics 2009-11-10 Silvia Vaulá

A noncommutative space is considered the position operators of which satisfy the commutativity relations of a Lie algebra. The basic tools for calculation on this space, including the product of the fields, inner product and the proper…

High Energy Physics - Theory · Physics 2008-11-26 A. H. Fatollahi , M. Khorrami

We investigate singly and doubly charged flux tubes in U(1) lattice gauge theory. By simulating the dually transformed path integral we are able to consider large flux tube lengths, low temperatures, and multiply charged systems without…

High Energy Physics - Lattice · Physics 2008-11-26 Martin Zach , Manfried Faber , Peter Skala

A detailed Monte Carlo calculation of the phase diagram of bosonic IKKT Yang-Mills matrix models in three and six dimensions with quartic mass deformations is given. Background emergent fuzzy geometries in two and four dimensions are…

High Energy Physics - Theory · Physics 2017-03-08 Badis Ydri , Rouag Ahlam , Ramda Khaled

A matrix model is constructed which describes a chiral version of the large $N$ $U(N)$ gauge theory on a two-dimensional sphere of area $A$. This theory has three separate phases. The large area phase describes the associated chiral string…

High Energy Physics - Theory · Physics 2009-10-28 M. Crescimanno , W. Taylor

In this manuscript we study the Double SU(4) model as a grand unified theory based on the gauge group $\,SU(4)\times SU(4)\left(\times \mathcal{Z}_2\right)$. A complete set of generators is constructed according to a pattern of symmetry…

High Energy Physics - Phenomenology · Physics 2019-03-11 Jose A. R. Cembranos , Pablo Diez-Valle

Many gauge theory models on fuzzy complex projective spaces will contain a strong instability in the quantum field theory leading to topology change. This can be thought of as due to the interaction between spacetime via its…

High Energy Physics - Theory · Physics 2008-11-26 Djamel Dou , Badis Ydri

We study the squared width and the profile of flux tubes in compact U(1) lattice gauge theory in three spacetime dimensions. The results obtained from numerical calculations in the dual formulation of this confining theory are compared with…

High Energy Physics - Lattice · Physics 2016-03-07 Michele Caselle , Marco Panero , Davide Vadacchino

We discuss a limit of 3d $T_\rho^\sigma[SU(N)]$ quiver gauge theories in which the number of nodes is large and the ranks scale quadratically with the length of the quiver. The sphere free energies and topologically twisted indices are…

High Energy Physics - Theory · Physics 2021-06-21 Lorenzo Coccia , Christoph F. Uhlemann

We start with an $SU(\cal {N})$ Yang-Mills theory on a manifold ${\cal M}$, suitably coupled to two distinct set of scalar fields in the adjoint representation of $SU({\cal N})$, which are forming a doublet and a triplet, respectively under…

High Energy Physics - Theory · Physics 2015-07-17 Seckin Kurkcuoglu