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Related papers: ElectroWeak Precision Observables at One-Loop in H…

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We present a simple new way to visualize the constraints of Higgs coupling measurements on light stops in natural SUSY scenarios beyond the MSSM, which works directly in the plane of stop mass eigenvalues (with no need to make assumptions…

High Energy Physics - Phenomenology · Physics 2015-06-18 JiJi Fan , Matthew Reece

Recent preliminary results obtained by the CDF and D0 Collaborations on searches for the Higgs boson in proton anti-proton collisions at Sqrt(s)=1.96 TeV at the Fermilab Tevatron collider are discussed. The data, corresponding to integrated…

High Energy Physics - Experiment · Physics 2007-06-12 Krisztian Peters

We present the current status of searches for a low mass Standard Model Higgs boson (M_H below ~ 135 GeV/c^2) using data collected from ppbar collisions at the Fermilab Tevatron collider at \sqrt{s}= 1.96 TeV. A summary of the latest…

High Energy Physics - Experiment · Physics 2019-08-14 Pierluigi Totaro

A search for anomalous pseudoscalar couplings of the Higgs boson H to electroweak vector bosons V (= W or Z) in a sample of proton-proton collision events corresponding to an integrated luminosity of 18.9 inverse femtobarns at a…

High Energy Physics - Experiment · Physics 2016-08-04 CMS Collaboration

Relatively light stops in gauge mediation models are usually made compatible with the Higgs mass of 125 GeV by introducing direct Higgs-messenger couplings. We show that such couplings are not necessary in a simple and predictive model that…

High Energy Physics - Phenomenology · Physics 2015-10-13 Ben Allanach , Marcin Badziak , Cyril Hugonie , Robert Ziegler

Composite Higgs models predict the existence of resonances. We study in detail the collider phenomenology of both the vector and fermionic resonances, including the possibility of both of them being light and within the reach of the LHC. We…

High Energy Physics - Phenomenology · Physics 2019-01-29 Da Liu , Lian-Tao Wang , Ke-Pan Xie

We perform an analysis of the electroweak precision observables in the Lee-Wick Standard Model. The most stringent restrictions come from the S and T parameters that receive important tree level and one loop contributions. In general the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ezequiel Alvarez , Leandro Da Rold , Carlos Schat , Alejandro Szynkman

The final state obtained when a Higgs boson decays to a photon and a Z boson has been mostly overlooked in current searches for a light Higgs boson. However, when the Z boson decays leptonically, all final state particles in this channel…

High Energy Physics - Phenomenology · Physics 2015-03-19 James S. Gainer , Wai-Yee Keung , Ian Low , Pedro Schwaller

We revisit the constraints on the parameter space of the Minimal Supersymmetric Standard Model (MSSM), from charge and color breaking minima in the light of information on the Higgs from the LHC so far. We study the behavior of the scalar…

High Energy Physics - Phenomenology · Physics 2017-04-25 Debtosh Chowdhury , Rohini M. Godbole , Kirtimaan A. Mohan , Sudhir K. Vempati

We explore the sensitivity of the LHC at 14 TeV centre-of-mass energy (LHC14) to the single production and decay of top-antitop resonances in the four-top final state. We focus on the same-sign dilepton channel, and work within a simplified…

High Energy Physics - Phenomenology · Physics 2016-05-25 Da Liu , Rakhi Mahbubani

In the Higgs search at the LHC, a light Higgs boson (115 GeV <~ M_H <~ 130 GeV) is not excluded by experimental data. In this mass range, the width of the Standard Model Higgs boson is more than four orders of magnitude smaller than its…

High Energy Physics - Phenomenology · Physics 2015-06-05 Nikolas Kauer , Giampiero Passarino

In this paper, we investigate how the LHC data limit the Higgs-related couplings in the effective description of a strongly interacting extension of the Standard model. The Higgs boson is introduced as a scalar composite state and it is…

High Energy Physics - Phenomenology · Physics 2016-12-12 Mikulas Gintner , Josef Juran

Simulation results are presented on Higgs mass calculations in the spontaneously broken phase of the Higgs sector in the minimal Standard Model with a higher derivative regulator. A heavy Higgs particle is found in the TeV mass range in the…

High Energy Physics - Lattice · Physics 2008-02-03 C. Liu , K. Jansen , J. Kuti

Electroweak precision observables (EWPO) can give valuable information about the last unknown paramter of the Standard Model (SM), the Higgs-boson mass M_H^SM. EWPO can also restrict the parameter space of new physics models (NPM) such as…

High Energy Physics - Phenomenology · Physics 2007-10-17 S. Heinemeyer

In 5 dimensions the electroweak symmetry can be broken by boundary conditions, leading to a new type of Higgsless theories. These could in principle improve on the 4D case by extending the perturbative domain to energies higher than $4 \pi…

High Energy Physics - Phenomenology · Physics 2008-11-26 Riccardo Barbieri , Alex Pomarol , Riccardo Rattazzi

The Standard Model (SM) with a light Higgs boson provides a very good description of the precision electroweak observable data coming from the LEP, SLD and Tevatron experiments. Most of the observables, with the notable exception of the…

High Energy Physics - Phenomenology · Physics 2010-04-06 D. Choudhury , T. M. P. Tait , C. E. M. Wagner

In the Standard Model (SM), the Higgs mass around 125 GeV implies that the electroweak vacuum is metastable since the quartic Higgs coupling turns negative at high energies. I point out that a tiny mixing of the Higgs with a heavy singlet…

High Energy Physics - Phenomenology · Physics 2015-06-04 Oleg Lebedev

In a general supersymmetric standard model there is an upper bound $m_h$ on the tree level mass of the $CP=+1$ lightest Higgs boson which depends on the electroweak scale, $\tan \beta$ and the gauge and Yukawa couplings of the theory. When…

High Energy Physics - Phenomenology · Physics 2009-10-22 J. R. Espinosa , M. Quirós

If there are no light Higgs bosons found below $\cal O$(800 GeV) or so, the interactions among longitudinally-polarized vector bosons ($\wl$) will become strong at the TeV region, and new physics that is responsible for the electroweak…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tao Han

Only small regions in the $m_{t} - \tan\beta$ plane are allowed when considering simultaneously (assuming the MSSM) coupling constant unification and (minimal) GUT relations among Yukawa couplings (i.e., $h_{b} = h_{\tau}$ at the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nir Polonsky