neutral gauge boson
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2020 ◽  
Vol 803 ◽  
pp. 135326
Author(s):  
Mohammad Abdullah ◽  
Mykhailo Dalchenko ◽  
Teruki Kamon ◽  
Denis Rathjens ◽  
Adrian Thompson

2018 ◽  
Vol 97 (11) ◽  
Author(s):  
Tyler Corbett ◽  
Matthew J. Dolan ◽  
Christoph Englert ◽  
Karl Nordström

2016 ◽  
Vol 31 (27) ◽  
pp. 1650159 ◽  
Author(s):  
Kunio Kaneta ◽  
Subeom Kang ◽  
Hye-Sung Lee

Recently there has been a huge interest in the diphoton excess around 750 GeV reported by both ATLAS and CMS collaborations, although the newest analysis with more statistics does not seem to support the excess. Nevertheless, the diphoton channel at the LHC experiments are a powerful tool to probe a new physics. One of the most natural explanations of a diphoton excess, if it occurs, could be a new scalar boson with exotic colored particles. In this setup, it would be legitimate to ask what is the role of this new scalar in nature. A heavy neutral gauge boson [Formula: see text] is one of the traditional targets of the discovery at the collider experiments with numerous motivations. While the Landau–Yang theorem dictates the diphoton excess cannot be this spin-1 gauge boson, there is a strong correlation of a new heavy gauge boson and a new scalar boson which provides a mass to the gauge boson being at the same mass scale. In this paper, we point out a simple fact that a new scalar with a property similar to the recently highlighted 750 GeV would suggest an existence of a TeV scale [Formula: see text] gauge boson that might be within the reach of the LHC Run 2 experiments. We take a scenario of the well-motivated and popular gauged [Formula: see text] symmetry and require the gauge coupling unification to predict the mass and other properties of the [Formula: see text] and illustrate the discovery of the [Formula: see text] would occur during the LHC experiments.


2015 ◽  
Vol 25 (1) ◽  
pp. 29 ◽  
Author(s):  
Dinh Thanh Binh ◽  
Do Thi Huong ◽  
Le Tho Hue ◽  
Hoang Ngoc Long

We investigate in detail  $one-loop$ contribution of new particles to the muon  anomalous magnetic moment \((g-2)_\mu\) in the framework of the economical 3-3-1 model. The main contributions to the anomalous magnetic moment come from new neutral gauge boson \(Z'\),  bilepton  singly charged  vector boson $Y^\pm$. The contributions of new neutral/charged scalars are small and can be neglected. The result is extended to other versions of 3-3-1 models.Comparing the anomalous magnetic moment value in this model with experimental value we set the extension requirement for the model.


2014 ◽  
Vol 24 (2) ◽  
pp. 97 ◽  
Author(s):  
Vu Thi Ngoc Huyen ◽  
Hoang Ngoc Long ◽  
Tran Thanh Lam ◽  
Vo Quoc Phong

This work is devoted for gauge boson sector of the recentlyproposed model based on \(\mathrm{SU}(3)_C\otimes \mathrm{SU}(3)_L\otimes \mathrm{U}(1)_X\) group with minimal content of leptons andHiggses. The limits on the masses of the bilepton gauge bosons andon the mixing angle among the neutral ones are deduced. Using theFritzsch anzats on quark mixing, we show that the third family ofquarks should  be different from the first two. We obtain a lowerbound on mass of the new heavy neutral gauge boson as 4.032 TeV.Using data on branching decay rates of the \(Z\) boson, we  can fix the limit to the \(Z\) and $Z^\prime$ mixing angle\(\phi\) as \(-0.001\le\phi\le 0.0003\).


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