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Related papers: Top mode standard model and extra dimensions

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We investigate the status of predictive fermion mass ansatzes which make use of the grand unification scale conditions $m_e=m_d/3$, $m_\mu =3m_s$, and $\mid V_{cb}\mid =\sqrt{m_{c}/m_{t}}$ in non-supersymmetric SO(10) grand unification. The…

High Energy Physics - Phenomenology · Physics 2010-11-01 N. G. Deshpande , E. Keith

The LHC discovery potential of heavy top partners decaying into a top quark and a $Z$ boson is studied in the trilepton channel at $\sqrt{s}=13$ TeV. The clean multilepton final state allows to strongly reduce the background contaminations…

High Energy Physics - Phenomenology · Physics 2015-02-11 Lorenzo Basso , Jeremy Andrea

We consider the maximal U(3) horizontal scheme as a handle on fermion masses and mixings. In particular, we attempt to explain the large top Yukawa coupling and the masses and mixing in the two heaviest generations. A simple model is…

High Energy Physics - Phenomenology · Physics 2016-08-25 Andrija Rasin

In a variety of well motivated models, such as two Higgs Doublet Models (2HDMs) and the Minimal Supersymmetric Standard Model (MSSM), there are neutral Higgs bosons that have significantly enhanced couplings to b-quarks and tau leptons in…

High Energy Physics - Phenomenology · Physics 2015-06-04 Marcela Carena , Stefania Gori , Aurelio Juste , Arjun Menon , Carlos E. M. Wagner , Lian-Tao Wang

Universal Extra Dimension (UED) models tend to favor a distinctively heavier Higgs mass than in the Standard Model (SM) and its supersymmetric extensions when the Kaluza-Klein (KK) scale is not much higher than the electroweak one, which we…

High Energy Physics - Phenomenology · Physics 2013-05-30 Kenji Nishiwaki , Kin-ya Oda , Naoya Okuda , Ryoutaro Watanabe

We review the model-independent description of the couplings of the top quark to the Higgs and gauge bosons in theories beyond the Standard Model. Then we examine these couplings in the case of arbitrary heavy vector-like quarks mixing with…

High Energy Physics - Phenomenology · Physics 2015-06-15 J. A. Aguilar-Saavedra , M. Perez-Victoria

We study the production of a Standard Model (SM) Higgs boson in association with a single top quark and either a light jet or $W$-boson at the LHC with a center of mass energy of 14 TeV. Due to the destructive interference of the…

High Energy Physics - Phenomenology · Physics 2010-05-12 Vernon Barger , Mathew McCaskey , Gabe Shaughnessy

Theories which provide a dynamical explanation for the large top-quark mass often include TeV-scale vector-like top-quark and bottom-quark partner states which can be potentially discovered at the LHC. These states are currently probed…

High Energy Physics - Phenomenology · Physics 2022-11-10 Alexander Belyaev , R. Sekhar Chivukula , Benjamin Fuks , Elizabeth H. Simmons , Xing Wang

Charged Higgs bosons heavier than the top quark and decaying via $H^{\pm} \rightarrow tb$ are searched for in proton--proton collisions measured with the ATLAS experiment at $\sqrt{s}=8$ TeV corresponding to an integrated luminosity of 20.3…

High Energy Physics - Experiment · Physics 2016-03-25 ATLAS Collaboration

We review and update current limits on possible anomalous couplings of the top quark to gauge bosons. We consider data from top quark decay (as encoded in the $W$-boson helicity fractions) and single-top production (in the $t$-, $s$- and…

High Energy Physics - Phenomenology · Physics 2014-06-23 M. Fabbrichesi , M. Pinamonti , A. Tonero

The top quark, being the heaviest elementary fermion known in the Standard model, has the largest coupling to the Higgs boson. The associated production of top quarks with the Higgs boson, either in pairs (t$\bar{\rm{t}}$H) or singly (tH),…

High Energy Physics - Experiment · Physics 2017-12-19 Georgios Konstantinos Krintiras

We discuss possible non-standard contributions to the top-quark width, particularly the virtual effects on the standard decay $t\rightarrow W^+\,b$ within the context of the MSSM. We also place a renewed emphasis on the unconventional mode…

High Energy Physics - Phenomenology · Physics 2008-02-03 Joan Sola

The precise knowledge of the Standard Model Higgs boson and top quark masses and couplings are crucial to understand the physics beyond it. SM like Higgs boson having mass in the range of 123-127 GeV squeezes the parameters for beyond…

High Energy Physics - Phenomenology · Physics 2014-04-03 Joydeep Chakrabortty , Partha Konar , Tanmoy Mondal

We measure the top quark mass in top-antitop events using up to 3.6 /fb of proton-antiproton collisions at sqrt{s}=2 TeV. New results are described for matrix element methods with single lepton and dilepton channels, and template methods…

High Energy Physics - Experiment · Physics 2019-08-14 R. L. Kehoe

It is shown that fine-tuning of the Higgs parameters stronger than a few % is required at the best in the models with gauge mediated supersymmetry breaking. With the aim of solving this problem, we consider a new type of models in which the…

High Energy Physics - Phenomenology · Physics 2011-01-13 Tatsuo Kobayashi , Haruhiko Terao , Akito Tsuchiya

A search for the Standard Model Higgs boson has been performed in the H \rightarrow WW \rightarrow l{\nu}jj channel in 1.04 fb-1 of pp collisions at \surds = 7 TeV collected with the ATLAS detector at the Large Hadron Collider. No…

High Energy Physics - Experiment · Physics 2019-08-13 Mark S. Neubauer

In the Standard Model with four generations, the two-loop renormalization group equations for the Higgs quartic and Yukawa couplings have a fixed point structure. If the masses of the fourth family are sufficiently heavy, it will contain a…

High Energy Physics - Phenomenology · Physics 2011-03-03 P. Q. Hung , Chi Xiong

Top-partners -- vector-like quarks which mix predominantly with the top quark -- are simple extensions of the standard model present in many theories of new physics such as little Higgs models, topcolor models, and extra dimensions. Through…

High Energy Physics - Phenomenology · Physics 2013-05-29 Graham D. Kribs , Adam Martin , Tuhin S. Roy

Top-quark decays are sensitive probes of light charged Higgs bosons ($H^\pm$) due to the sizable $t\bar t$ production cross section at the LHC in conjunction with their distinct experimental signatures. While dedicated ATLAS and CMS…

High Energy Physics - Phenomenology · Physics 2026-04-23 Saiyad Ashanujjaman , Andreas Crivellin , Siddharth P. Maharathy , Bruce Mellado

First observed in 1995, the top quark is one of a pair of third-generation quarks in the Standard Model of particle physics. It has charge +2/3e and a mass of 171.4 GeV, about 40 times heavier than its partner, the bottom quark. The CDF and…

High Energy Physics - Experiment · Physics 2019-08-15 A. P. Heinson
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