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The SU(3) simplest little Higgs model in its original framework without the so-called mu term inevitably involves a massless pseudoscalar boson eta, which is problematic for b-physics and cosmological axion limit. With the mu term…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kingman Cheung , Jeonghyeon Song

We revisit the neutral Higgs sector of the Higgs Triplet Model, with non-negligible mixing in the CP-even Higgs sector. We examine the possibility that one of the Higgs boson state is the particle observed at the LHC at 125 GeV, and the…

High Energy Physics - Phenomenology · Physics 2013-05-30 Fatemeh Arbabifar , Sahar Bahrami , Mariana Frank

In the minimal supersymmetric Standard Model, the heaviest CP-even Higgs boson H and the CP-odd Higgs scalar A are predicted to be almost degenerate in mass at the tree level, for the wide kinematic range M_A > 2M_Z and \tan\beta \ge 2.…

High Energy Physics - Phenomenology · Physics 2011-01-27 Apostolos Pilaftsis

The simplest supersymmetric model that solves the mu problem and in which the GUT-scale parameters need not be finely tuned in order to predict the correct value of the Z boson mass at low scales is the Next-to-Minimal Supersymmetric…

High Energy Physics - Phenomenology · Physics 2009-02-18 J. R. Forshaw , J. F. Gunion , L. Hodgkinson , A. Papaefstathiou , A. D. Pilkington

The mass of the eta_b(1S), measured recently by BABAR, is significantly lower than expected from QCD predictions for the Upsilon(1S) - eta_b(1S) hyperfine splitting. We suggest that the observed eta_b(1S) mass is shifted downwards due to a…

High Energy Physics - Phenomenology · Physics 2009-12-07 Florian Domingo , Ulrich Ellwanger , Miguel-Angel Sanchis-Lozano

We show that the branching ratio R_{b/tau}=BR(h^0->bb)/BR(h^0->tau tau) of the Higgs boson h^0 may usefully differentiate between the Higgs sectors of the Minimal Supersymmetric Standard Model (MSSM) and non-supersymmetric models such as…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. S. Babu , Christopher Kolda

The generalization of the MSSM to the case of four chiral fermion generations (4GMSSM) can lead to significant changes in the phenomenology of the otherwise familiar Higgs sector. In most of the 3GMSSM parameter space, the lighter CP-even…

High Energy Physics - Phenomenology · Physics 2013-05-29 R. C. Cotta , J. L. Hewett , A. Ismail , M. -P. Le , T. G. Rizzo

In the CMSSM the heaviest scalar and pseudo-scalar Higgs bosons decay largely into b-quarks and tau-leptons because of the large $\tan\beta$ values favored by the relic density. In the NMSSM the number of possible decay modes is much…

High Energy Physics - Phenomenology · Physics 2016-07-13 C. Beskidt , W. de Boer , D. I. Kazakov , S. Wayand

This paper investigates the impact of the recent LHC constraints on the Higgs sector in the semi-constrained version of the Next-to-Minimal Supersymmetric Standard Model. Our analysis focuses on the parameter space for which the value of…

High Energy Physics - Phenomenology · Physics 2021-06-29 Marwa Telba , Maien Binjonaid

A search has been performed on 683 pb$^{-1}$ of data collected by the ALEPH detector at the Large Electron-Positron (LEP), collider at centre-of-mass energies from 183 to 209 $\mathrm{GeV}$ looking for a Higgs boson decaying into four…

High Energy Physics - Experiment · Physics 2010-06-15 James Beacham

A search for neutral Higgs bosons decaying to tau pairs at a center-of-mass energy of 7 TeV is performed using a dataset corresponding to an integrated luminosity of 4.6 inverse femtobarns recorded by the CMS experiment at the LHC. The…

High Energy Physics - Experiment · Physics 2014-11-14 CMS Collaboration

We study the invisible decay of the Higgs boson into a pair of stable, heavy photons, H -> A_H A_H, in the littlest Higgs model with T-parity. For a symmetry breaking scale of f = 450 GeV, the branching ratio H -> A_H A_H can be as high as…

High Energy Physics - Phenomenology · Physics 2008-11-26 Raghavendra Srikanth Hundi , Biswarup Mukhopadhyaya , Andreas Nyffeler

We explore the possibility that physics at the TeV scale possesses approximate $N = 2$ supersymmetry, which is reduced to the $N=1$ minimal supersymmetric extension of the Standard Model (MSSM) at the electroweak scale. This doubling of…

High Energy Physics - Phenomenology · Physics 2016-11-23 John Ellis , Jérémie Quevillon , Verónica Sanz

Naturalness of electroweak symmetry breaking in the next-to-minimal supersymmetric model points to scenarios in which the lightest CP-even Higgs boson has SM-like ZZh coupling and mass m_h ~ 100 GeV and decays partly via h -> b \bar b but…

High Energy Physics - Phenomenology · Physics 2008-11-26 Radovan Dermisek , John F. Gunion

A search for the Standard Model Higgs boson decaying into a pair of tau leptons is reported. The analysis is based on a data sample of proton-proton collisions collected by the ATLAS experiment at the LHC and corresponding to an integrated…

High Energy Physics - Experiment · Physics 2013-06-11 ATLAS Collaboration

A search for the production and non-standard decay of a Higgs boson, h, into four taus through intermediate pseudoscalars, a, is conducted on 683 pb-1 of data collected by the ALEPH experiment at centre-of-mass energies from 183 to 209 GeV.…

High Energy Physics - Experiment · Physics 2016-08-14 ALEPH Collaboration , S. Schael , R. Barate , R. Brunelière , I. De Bonis , D. Decamp , C. Goy , S. Jézéquel , J. -P. Lees , F. Martin , E. Merle , M. -N. Minard , B. Pietrzyk , B. Trocmé S. Bravo , M. P. Casado , M. Chmeissani , J. M. Crespo , E. Fernandez , M. Fernandez-Bosman , Ll. Garrido , M. Martinez , A. Pacheco , H. Ruiz , A. Colaleo , D. Creanza , N. De Filippis , M. de Palma , G. Iaselli , G. Maggi , M. Maggi , S. Nuzzo , A. Ranieri , G. Raso , F. Ruggieri , G. Selvaggi , L. Silvestris , P. Tempesta , A. Tricomi , G. Zito X. Huang , J. Lin , Q. Ouyang , T. Wang , Y. Xie , R. Xu , S. Xue , J. Zhang , L. Zhang , W. Zhao , D. Abbaneo , T. Barklow , O. Buchmüller , M. Cattaneo , B. Clerbaux , H. Drevermann , R. W. Forty , M. Frank , F. Gianotti , J. B. Hansen , J. Harvey , D. E. Hutchcroft , P. Janot , B. Jost , M. Kado , P. Mato , A. Moutoussi , F. Ranjard , L. Rolandi , D. Schlatter , F. Teubert , A. Valassi , I. Videau S. Monteil , D. Pallin , J. M. Pascolo , P. Perret , J. D. Hansen , J. R. Hansen , P. H. Hansen , A. C. Kraan , B. S. Nilsson A. Kyriakis , C. Markou , E. Simopoulou , A. Vayaki , K. Zachariadou A. Blondel , J. -C. Brient , F. Machefert , A. Rougé , H. Videau , V. Ciulli , E. Focardi , G. Parrini , A. Antonelli , M. Antonelli , G. Bencivenni , F. Bossi , G. Capon , F. Cerutti , V. Chiarella , P. Laurelli , G. Mannocchi , G. P. Murtas , L. Passalacqua , J. Kennedy , J. G. Lynch , P. Negus , V. O'Shea , A. S. Thompson , R. Cavanaugh , S. Dhamotharan , C. Geweniger , P. Hanke , V. Hepp , E. E. Kluge , A. Putzer , H. Stenzel , K. Tittel , M. Wunsch , R. Beuselinck , W. Cameron , G. Davies , P. J. Dornan , M. Girone , N. Marinelli , J. Nowell , S. A. Rutherford , J. K. Sedgbeer , J. C. Thompson , R. White , V. M. Ghete , P. Girtler , E. Kneringer , D. Kuhn , G. Rudolph , E. Bouhova-Thacker , C. K. Bowdery , D. P. Clarke , G. Ellis , A. J. Finch , F. Foster , G. Hughes , R. W. L. Jones , M. R. Pearson , N. A. Robertson , T. Sloan , M. Smizanska , O. van der Aa , C. Delaere , G. Leibenguth , V. Lemaitre U. Blumenschein , F. Hölldorfer , K. Jakobs , F. Kayser , A. -S. Müller , B. Renk , H. -G. Sander , S. Schmeling , H. Wachsmuth , C. Zeitnitz , T. Ziegler A. Bonissent , P. Coyle , C. Curtil , A. Ealet , D. Fouchez , P. Payre , A. Tilquin , F. Ragusa , A. David , H. Dietl , G. Ganis , K. Hüttmann , G. Lütjens , W. Männer H. -G. Moser , R. Settles , M. Villegas , G. Wolf , J. Beacham , K. Cranmer I. Yavin , J. Boucrot , O. Callot , M. Davier , L. Duflot , J. -F. Grivaz , Ph. Heusse , A. Jacholkowska , L. Serin , J. -J. Veille , P. Azzurri , G. Bagliesi , T. Boccali , L. Foà , A. Giammanco , A. Giassi , F. Ligabue , A. Messineo , F. Palla , G. Sanguinetti , A. Sciabà , G. Sguazzoni , P. Spagnolo , R. Tenchini , A. Venturi , P. G. Verdini O. Awunor , G. A. Blair , G. Cowan , A. Garcia-Bellido , M. G. Green , T. Medcalf , A. Misiejuk , J. A. Strong , P. Teixeira-Dias , R. W. Clifft , T. R. Edgecock , P. R. Norton , I. R. Tomalin , J. J. Ward B. Bloch-Devaux , D. Boumediene , P. Colas , B. Fabbro , E. Lançon , M. -C. Lemaire , E. Locci , P. Perez , J. Rander , B. Tuchming , B. Vallage , A. M. Litke , G. Taylor , C. N. Booth , S. Cartwright , F. Combley , P. N. Hodgson , M. Lehto , L. F. Thompson , A. Böhrer , S. Brandt , C. Grupen , J. Hess , A. Ngac , G. Prange C. Borean , G. Giannini , H. He , J. Putz , J. Rothberg , S. R. Armstrong , K. Berkelman , D. P. S. Ferguson , Y. Gao , S. González , O. J. Hayes , H. Hu , S. Jin , J. Kile , P. A. McNamara , J. Nielsen , Y. B. Pan , J. H. von Wimmersperg-Toeller , W. Wiedenmann , J. Wu , Sau Lan Wu , X. Wu , G. Zobernig , G. Dissertori

We investigate the impact of electroweak (EW), scalar and QCD corrections to the full set of decay branching ratios of an additional CP-even Higgs boson ($H$) in the two Higgs doublet model with a softly broken $Z_2$ symmetry. We employ the…

High Energy Physics - Phenomenology · Physics 2022-08-10 Shinya Kanemura , Mariko Kikuchi , Kei Yagyu

An accurate determination of the Higgs decay branching ratios to bb, cc, gg, WW* and tau tau pairs is important for the study of the Higgs couplings and for determining its SM or MSSM nature in the mass range 100 GeV/c2 < M_H < 140 GeV/c^2.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marco Battaglia

The Next to Minimal Supersymmetric Standard Model (NMSSM) with a Higgs-singlet coupling {\lambda} close to unity, moderate tan {\beta} and stop masses below 1 TeV minimizes the fine tuning of the electroweak scale, making possible that the…

High Energy Physics - Phenomenology · Physics 2013-06-25 Riccardo Barbieri , Dario Buttazzo , Kristjan Kannike , Filippo Sala , Andrea Tesi

This paper presents a search for Higgs bosons decaying to four leptons, either electrons or muons, via one or two light exotic gauge bosons $Z_d$, $H\to Z Z_d \to 4\ell$ or $H\to Z_d Z_d \to 4\ell$. The search was performed using $pp$…

High Energy Physics - Experiment · Physics 2015-11-11 ATLAS Collaboration
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