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Related papers: Neutral currents in reduced minimal 3-3-1 model

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The 1-loop renormalization group equations for the minimal Z' models encompassing a type-I seesaw mechanism are studied in the light of the 125 GeV Higgs boson discovery. This model is taken as a benchmark for the general case of singlet…

High Energy Physics - Phenomenology · Physics 2014-01-30 Lorenzo Basso

We perform a comprehensive analysis of the secluded UMSSM model, consistent with present experimental constraints. We find that in this model the additional $Z^\prime$ gauge boson can be leptophobic without resorting to gauge kinetic mixing…

High Energy Physics - Phenomenology · Physics 2020-12-24 Mariana Frank , Yaşar Hiçyılmaz , Stefano Moretti , Özer Özdal

We obtain mass limits on the extra neutral gauge boson which is predicted in a model with hidden gauge symmetry and dynamical breaking of the electroweak symmetry by a top quark condensate. For typical model assumptions, present LEP data…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ralf Bönisch , Arnd Leike

We study a new class of flavor changing interactions, which can arise in models based on extended gauge groups (rank $>$4) when new charged fermions are present together with a new neutral gauge boson. We discuss the cases in which the…

High Energy Physics - Phenomenology · Physics 2009-10-22 E. Nardi

Spectra, triple and quartic gauge couplings of the Higgsless model with gauge group $SU(2)_L\times SU(2)_R\times U(1)_{B-L}$ defined in warped space are explored with numerical method. We extend the equation of motions, boundary conditions…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kingman Cheung , Xiao-Hong Wu , Qi-Shu Yan

An extension of the gauge group $SU(2)_L\otimes U(1)_Y$ of the standard model to the symmetry group $SU(4)_L\otimes U(1)_X$ (3-4-1 for short) is presented. The model does not contain exotic electric charges and anomaly cancellation is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Luis A. Sanchez , Luis A. Wills-Toro , Jorge I. Zuluaga

The parity violation in cesium atom is analysed in the framework of the models based on the SU(3)_C X SU(3)_L X U(1)_N gauge group. It is shown that in the minimal version, the main contribution to a deviation of weak charge \Delta Q_W due…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hoang Ngoc Long , Le Phuoc Trung

The phenomenology of an additional U(1) neutral gauge boson Z' coupled to the third family of fermions is discussed. One might expect such a particle to contribute to processes where taus, b and t quarks are produced. Precision data from…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. A. Andrianov , P. Osland , A. A. Pankov , N. V. Romanenko , J. Sirkka

$Z^\prime$ boson as a new gauge boson has been proposed in many new physics models. The interactions of $Z^\prime$ coupling to fermions are detailed studied at the large hadron collider. A $Z^\prime$ with the mass of a few TeV has been…

High Energy Physics - Phenomenology · Physics 2022-05-11 Xinyue Yin , Honglei Li , Yi Jin , Zhilong Han , Zongyang Lu

In supersymmetric $E_6$ the masses of the third family quarks and charged lepton, $t-b-\tau$, as well as the masses of the vector-like quarks and leptons, $D-\bar{D}$ and $ L-\bar{L}$, may arise from the coupling $27_3$ x $27_3$ x $27_H$,…

High Energy Physics - Phenomenology · Physics 2016-06-22 Aditya Hebbar , George K. Leontaris , Qaisar Shafi

We point out that the stringent lower bounds on the masses of additional electrically neutral and charged Higgs bosons crucially depend on the flavour structure of their Yukawa interactions. We show that these bounds can easily be evaded by…

High Energy Physics - Phenomenology · Physics 2018-03-28 Stefania Gori , Christophe Grojean , Aurelio Juste , Ayan Paul

We discuss a new SU(3)_C X SU(3)_L X U(1)_X X U(1)_N (3-3-1-1) gauge model that overhauls the theoretical and phenomenological aspects of the known 3-3-1 models. Additionally, we sift the outcome of the 3-3-1-1 model from precise…

High Energy Physics - Phenomenology · Physics 2014-10-28 P. V. Dong , D. T. Huong , Farinaldo S. Queiroz , N. T. Thuy

We present the study of the quark sector of the universal seesaw model with $\mathrm{SU(2)_L \times SU(2)_R \times U(1)_{Y'}}$ gauge symmetry in the massless case of the two lightest quark families. This model aims to explain the mass…

High Energy Physics - Phenomenology · Physics 2024-09-19 Takuya Morozumi , Albertus Hariwangsa Panuluh

Motivated by a recent rather surprising conclusion based on the 1992 PDG data on the pion, kaon and lepton decays that if three generations of neutrinos are assumed to be massive and mixed, the heaviest neutrino, $\nu_3$, could have a mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Bottino , N. Fornengo , C. W. Kim , G. Mignola

We consider an extended electroweak gauge group: SU(2)$_1 \times$ SU(2)$_2 \times$ U(1)$_Y$ where the first and second generation of fermions couple to SU(2)$_1$ and the third generation couples to SU(2)$_2$. Bounds based on heavy gauge…

High Energy Physics - Phenomenology · Physics 2010-12-02 David Muller , Satyanarayan Nandi

In this note I mainly focus on the neutrino physics part in my talk and report the most recent progress made in \cite{YLW0}. It is seen that the Majorana features of neutrinos and SO(3) gauge flavor symmetry can simultaneously explain the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yue-Liang Wu

It was recently shown that left-right symmetric models for elementary particles can be built with only two Higgs doublets. The general consequence of these models is that the left and right fermionic sectors can be connected by a new…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. M. L. Almeida , Y. A. Coutinho , J. A. Martins Simões , J. Ponciano , A. J. Ramalho , Stenio Wulck , M. A. B. Vale

By adding new gauge singlets of neutral leptons, the improved versions of the 3-3-1 models with right-handed neutrinos have been recently introduced in order to explain recent experimental neutrino oscillation data through the inverse…

High Energy Physics - Phenomenology · Physics 2018-04-18 T. Phong Nguyen , T. Thuy Le , T. T. Hong , L. T. Hue

Limits on the Higgs boson mass restrict CKM mixing of a possible fourth family beyond the constraints previously obtained from precision electroweak data alone. Existing experimental and theoretical bounds on the Higgs mass already…

High Energy Physics - Phenomenology · Physics 2014-11-21 Michael S. Chanowitz

We calculate radiative corrections to the masses of the Higgs bosons in a minimal supersymmetric model that contains an additional non-anomalous (U(1)') gauge symmetry. With some fine-tuning of the (U(1)') charges of the Higgs fields, it is…

High Energy Physics - Phenomenology · Physics 2009-11-07 Hassib Amini
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