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Related papers: Mass-deformed $T_N$ as a linear quiver

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A gauge theory with an underlying SU_q(2) quantum group symmetry is introduced, and its properties examined. With suitable assumptions, this model is found to have many similarities with the usual SU(2)\times U(1) Standard Model,…

High Energy Physics - Theory · Physics 2009-10-30 Paul Watts

We study the interplay between mass deformations and unoriented projections of super-conformal quiver gauge theories resulting from D3-branes at (toric) Calabi-Yau singularities. We focus on simple orbifold cases…

High Energy Physics - Theory · Physics 2020-07-28 Massimo Bianchi , Davide Bufalini , Salvo Mancani , Fabio Riccioni

We study a possibility to explain neutrino masses and mixings based on supersymmetry. If we introduce a flavor diagonal but generation dependent extra U(1) gauge interaction at a TeV region, we can obtain masses and mixings of neutrinos…

High Energy Physics - Phenomenology · Physics 2007-05-23 Daijiro Suematsu

In this paper, we continue the study of $T\bar{T}$ deformation in $d=1$ quantum mechanical systems and propose possible analogues of $J\bar{T}$ deformation and deformation by a general linear combination of $T\bar{T}$ and $J\bar{T}$ in…

High Energy Physics - Theory · Physics 2020-12-30 Soumangsu Chakraborty , Amiya Mishra

We show that Seiberg-like duality of $\mathcal{N}=1$ gauge theory coupled with tensor chiral fields and fundamental chiral fields works if the meson spectrum built from the tensor fields takes particular form: a) It should be truncated; b)…

High Energy Physics - Theory · Physics 2024-03-05 Yuanyuan Fang , Jing Feng , Dan Xie

We consider the possibility that QCD with N flavors has a useful low-energy description with 2N flavors. Specifically, we investigate a free theory of 2N quarks. Although the free theory is U(N)_L X U(N)_R invariant, it admits a larger…

High Energy Physics - Phenomenology · Physics 2014-11-17 Silas R. Beane

The appearance of a broken supersymmetric U(1) gauge factor at the TeV scale is relevant for several reasons. If it truly exists, then one important consequence is that at the 100 GeV energy scale, the two-doublet Higgs structure is of a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ernest Ma

We consider the ${\cal N}=1$ $SU(N_c)$ SQCD-like (direct) theory (and its Seiberg's dual with $SU(N_F-N_c)$ dual colors), and with $N_F$ flavors of light quarks ${\overline Q}_j, Q^i$ with the mass term in the superpotential $m_Q{\rm…

High Energy Physics - Theory · Physics 2020-10-06 Victor L. Chernyak

We explore the consequences of assuming that the neutrino mass matrix is a linear combination of the matrices of a three dimensional representation of the group $S_3$ and that it has one zero mass eigenvalue. When implemented, these two…

High Energy Physics - Phenomenology · Physics 2014-11-20 Duane A. Dicus , Shao-Feng Ge , Wayne W. Repko

We extend a known mass-gap equation for pure gluodynamics in global colour models (formulated in equal time quantization in Coulomb gauge) to one in which gluons split into two sets which may have different masses. If the theory is…

High Energy Physics - Phenomenology · Physics 2025-05-30 Julia Gómez Concejo , Felipe J. Llanes-Estrada , Diego María-Almazán , Alexandre Salas-Bernárdez

We study five-dimensional ${\cal N}=1$ Superconformal Field Theories of the linear quiver type. These are deformed by a relevant operator, corresponding to a homogeneous mass term for certain matter fields. The free energy is calculated at…

High Energy Physics - Theory · Physics 2023-09-11 Mohammad Akhond , Andrea Legramandi , Carlos Nunez , Leonardo Santilli , Lucas Schepers

Solar neutrino problem and atmospheric neutrino anomaly which are both long-standing issues studied intensively by physicists in the past several decades, are reckoned to be able to be solved simultaneously in the framework of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shao-Xia Chen , Zhao-Yu Yang

We show that applying the Bailey lemma to elliptic hypergeometric integrals on the $A_n$ root system leads to a large web of dualities for $\mathcal{N} = 1$ supersymmetric linear quiver theories. The superconformal index of Seiberg's SQCD…

High Energy Physics - Theory · Physics 2016-12-08 Frederic Brünner , Vyacheslav P. Spiridonov

We construct a flavor model in an anti-SU(5) GUT with a tetrahedral symmetry $A_4$. We choose a basis where $Q_{text{em}}=-\frac13$ quarks and charged leptons are already mass eigenstates. This choice is possible from the $A_4$ symmetry.…

High Energy Physics - Phenomenology · Physics 2020-03-25 Paul H. Frampton , Jihn E. Kim , Se-Jin Kim , Soonkeon Nam

We consider N=1 supersymmetric gauge theories based on the group SU(N)_1 x SU(N)_2 x ... x SU(N)_k with matter content (N,N*,1,...,1) + (1,N,N*,...,1) + >... + (N*,1,1,...,N) as candidates for the unification symmetry of all particles. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernest Ma , Myriam Mondragon , G. Zoupanos

We present general formulae for the TsT transformation (T-duality, shift, T-duality) of type II string backgrounds and open string boundary conditions. The TsT transformation provides a systematic procedure to find string theory duals of…

High Energy Physics - Theory · Physics 2009-12-07 Emiliano Imeroni

Starting from the $\mathcal{N}=2$ SYM$_{4}$ quiver theory living on wrapped $% N_{i}D5$ branes around $S_{i}^{2}$ spheres of deformed ADE fibered Calabi-Yau threefolds (CY3) and considering deformations using \textit{% massive} vector…

High Energy Physics - Theory · Physics 2015-06-26 Malika Ait Benhaddou , El Hassan Saidi

The N=1 supersymmetric gauge SU(5) theory with one antisymmetric tensor, n+3 fundamentals and n+4 antifundamentals has dual magnetic descriptions in the infrared. By introducing extra singlet fields and tree level superpotential terms to…

High Energy Physics - Theory · Physics 2008-02-03 Chih-Lung Chou

We consider pure SU(N) gauge theories defined on an orbifold lattice, analogous to the S^1/Z_2 gauge theory orbifolds of the continuum, which according to the perturbative analysis do not have a Higgs phase. Non-perturbatively the…

High Energy Physics - Lattice · Physics 2015-06-18 Nikos Irges , Francesco Knechtli

The $D_4$ flavor model based on $\mathrm{SU}(3)_C \otimes \mathrm{SU}(3)_L \otimes \mathrm{U}(1)_X$ gauge symmetry that aims at describing quark mass and mixing is updated. After spontaneous breaking of flavor symmetry, with the constraint…

High Energy Physics - Phenomenology · Physics 2015-07-30 V. V. Vien , H. N. Long