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A remarkable U(1) gauge extension of the supersymmetric standard model was proposed eight years ago. It is anomaly-free, has no mu term, and conserves baryon and lepton numbers automatically. The phenomenology of a specific version of this…

High Energy Physics - Phenomenology · Physics 2010-05-19 Ernest Ma

Bounds of the neutral current sector parameters of the left-right symmetric model are investigated taking into account the low-energy data, LEP-data and CDF-result for the top mass $m_t=174\pm 10^{+13}_{-12}$. It is found that in the case…

High Energy Physics - Phenomenology · Physics 2009-10-28 J. Sirkka

Recently we proposed a TeV-scale Supersymmetric Standard Model in which the gauge coupling unification is as precise (at one loop) as in the MSSM, and occurs in the TeV range. One of the key ingredients of this model is the presence of new…

High Energy Physics - Theory · Physics 2009-10-31 Zurab Kakushadze

We present a supersymmetric grand unification scheme based on the gauge group SU(3)_c X SU(3)_L X SU(3)_R in which the proton and the lightest supersymmetric particle are stable, neutrinos are necessarily massive, and the observed baryon…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. Lazarides , C. Panagiotakopoulos , Q. Shafi

We present a framework of dark- and visible-sector unification in the E6 embedding of the standard model. The demand for consistently getting the standard model leads to the existence of the dark-sector. We show that the hierarchy of vevs…

High Energy Physics - Phenomenology · Physics 2025-11-19 Triparno Bandyopadhyay , Rinku Maji

We examine unification of gauge couplings in four dimensional renormalizable gauge theories inspired by the latticized (deconstructed) SM or MSSM in five dimensions. The models are based on replicated gauge groups, spontaneously broken to…

High Energy Physics - Phenomenology · Physics 2014-11-17 Piotr H. Chankowski , Adam Falkowski , Stefan Pokorski

We show that left-right symmetric models can easily accommodate stable TeV-scale dark matter particles without the need for an ad-hoc stabilizing symmetry. The stability of a newly introduced multiplet arises either accidentally as in the…

High Energy Physics - Phenomenology · Physics 2015-09-21 Julian Heeck , Sudhanwa Patra

We suggest a U(1)' gauge symmetry as an alternative to the usual R-parity of supersymmetric standard models, showing that it can also work as a common source of stabilities of proton and dark matter in addition to other attractive features.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hye-Sung Lee

Perturbative gauge coupling unification in realistic superstring models suggests the existence of additional heavy down-type quarks, beyond the minimal supersymmetric standard model. The mass scale of the heavy down-type quarks is…

High Energy Physics - Phenomenology · Physics 2009-10-28 Sanghyeon Chang , Claudio Coriano , Alon E. Faraggi

We perform a detailed study of the grand unified theories $SO(10)$ and $E(6)$ with left-right intermediate gauge symmetries of the form $SU(N)_L\otimes SU(N)_R \otimes \mathcal{G}$. Proton decay lifetime constrains the unification scale to…

High Energy Physics - Phenomenology · Physics 2018-05-16 Joydeep Chakrabortty , Rinku Maji , Subhendra Mohanty , Sunando Kumar Patra , Tripurari Srivastava

We consider a supersymmetric extension of quantum gauge theory based on a vector multiplet containing supersymmetric partners of spin 3/2 for the vector fields. The constructions of the model follows closely the usual construction of gauge…

High Energy Physics - Theory · Physics 2009-11-07 Dan Radu Grigore , Gunter Scharf

Supersymmetry is one of the best motivated new physics scenarios. To build a realistic supersymmetric standard model, however, a companion symmetry is necessary to address various issues. While R-parity is a popular candidate that can…

High Energy Physics - Phenomenology · Physics 2009-02-05 Hye-Sung Lee

We build a supersymmetric version with $SU(3)_C\otimes SU(2)_L\otimes U(1)_{Y^\prime}\otimes U(1)_{B-L}$ gauge symmetry, where $Y^\prime$ is a new charge and $B$ and $L$ are the usual baryonic and leptonic numbers. The model has three…

High Energy Physics - Phenomenology · Physics 2017-06-14 J. C. Montero , V. Pleitez , M. C. Rodriguez , B. L. Sánchez-Vega

We construct and discuss a 6D supersymmetric gauge theory involving four derivatives in the action. The theory involves a dimensionless coupling constant and is renormalizable. At the tree level, it enjoys N = (1,0) superconformal symmetry,…

High Energy Physics - Theory · Physics 2019-07-08 E. A. Ivanov , A. V. Smilga , B. M. Zupnik

The relevant phenomenology and the best search schemes of a subelectroweak-scale gauge boson can be vastly different depending on its coupling. For instance, the rare decay into a light gauge boson and the high precision parity test can be…

High Energy Physics - Phenomenology · Physics 2016-06-29 Hye-Sung Lee , Seokhoon Yun

A model of dark energy and dark matter was proposed earlier by one of us (PQH) which involved an unbroken gauge group $SU(2)_Z$ whose coupling $\alpha_Z \equiv g_Z^2/4 \pi\sim O(1)$ at a scale $\Lambda_Z \sim 3 \times 10^{-3} eV$ starting…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Q. Hung , Paola Mosconi

We study grand unified models in the five-dimensional space-time where the extra dimension is compactified on $S^1/Z_2$. The spontaneous breaking of unified gauge symmetries is achieved via vacuum expectation values of the extra-dimensional…

High Energy Physics - Phenomenology · Physics 2017-06-28 Kentaro Kojima , Kazunori Takenaga , Toshifumi Yamashita

We consider candidates for dark matter in models of gauge mediated supersymmetry breaking, in which the supersymmetry breaking sector is weakly coupled and calculable. Such models typically contain classically flat directions, that receive…

High Energy Physics - Phenomenology · Physics 2009-09-28 Boaz Keren-Zur , Luca Mazzucato , Yaron Oz

We explore the possibility of unification of gauge couplings near the Planck scale in models of extended technicolor. We observe that models of the form G X SU(3)_c X SU(2)_L X U(1)_Y cannot be realized, due to the presence of massless…

High Energy Physics - Phenomenology · Physics 2013-11-13 Joseph D. Lykken , Scott Willenbrock

Our contribution sets out to investigate the phenomenology of a gauge model based on an $SU_{L}(2) \times U_{R}(1)_{J} \times U(1)_{K}$-symmetry group. The model can accommodate in its distinct phases - by virtue of different…

High Energy Physics - Phenomenology · Physics 2018-02-19 M. J. Neves , J. A. Helayël-Neto
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