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The discovery of the Higgs boson suggests that also neutrinos get their mass from spontaneous symmetry breaking. In the simplest ungauged lepton number scheme, the Standard Model (SM) Higgs has now two other partners: a massive CP-even, as…

High Energy Physics - Phenomenology · Physics 2015-07-01 Cesar Bonilla , Jorge C. Romão , Jose W. F. Valle

The data collected by the OPAL experiment at sqrts=183 GeV were used to search for Higgs bosons which are predicted by the Standard Model and various extensions, such as general models with two Higgs field doublets and the Minimal…

High Energy Physics - Experiment · Physics 2008-11-26 The OPAL Collaboration , G. Abbiendi et al

The Standard Model Higgs boson is searched for in 233.2 pb-1 of data collected by the L3 detector at centre of mass energies from 192 GeV to 202 GeV. These data are consistent with the expectations of Standard Model processes and no…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

The ATLAS and CMS experiments have recently announced the discovery of a Higgs-like resonance with mass close to 125 GeV. Overall, the data is consistent with a Standard Model (SM)-like Higgs boson. Such a particle may arise in the minimal…

High Energy Physics - Phenomenology · Physics 2015-06-15 Marcela Carena , Stefania Gori , Nausheen R. Shah , Carlos E. M. Wagner , Lian-Tao Wang

Neutrino mass generation through the Higgs mechanism not only suggests the need to reconsider the physics of electroweak symmetry breaking from a new perspective, but also provides a new theoretically consistent and experimentally viable…

High Energy Physics - Phenomenology · Physics 2016-04-06 Cesar Bonilla , Jorge C. Romão , José W. F. Valle

A direct search for Higgs bosons produced via vector-boson fusion and subsequently decaying into invisible particles is reported. The analysis uses 139 $\text{fb}^{-1}$ of $pp$ collision data at a centre-of-mass energy of $\sqrt{s}$=13…

High Energy Physics - Experiment · Physics 2022-08-18 ATLAS Collaboration

We investigate the scalar sector in an extension of the Minimal Supersymmetric Standard Model (MSSM) containing a $SU(2)$ Higgs triplet of zero hypercharge and a gauge singlet beside the $SU(2)$ scalar doublets. In particular, we focus on a…

High Energy Physics - Phenomenology · Physics 2016-01-27 Priyotosh Bandyopadhyay , Claudio Coriano , Antonio Costantini

We study the mass spectra, production and decay properties of the lightest supersymmetric CP-even and CP-odd Higgs bosons in models with spontaneously broken R-parity (SBRP). We compare the resulting mass spectra with expectations of the…

High Energy Physics - Phenomenology · Physics 2009-06-25 M. Hirsch , J. C. Romao , J. W. F. Valle , A. Villanova del Moral

New light bosons that couple weakly to the standard model (SM) particles are predicted in various extensions of the standard model (BSM). Examples include supersymmetric (SUSY) theories with extended Higgs sectors or with a hidden valleys…

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

The mass and the decay width of a Higgs boson in the minimal standard model are evaluated by a variational method in the limit of strong self-coupling interaction. The non-perturbative technique provides an interpolation scheme between…

High Energy Physics - Phenomenology · Physics 2010-12-17 Fabio Siringo

The recent discovery of a Higgs-like boson at the LHC with a mass of 126 GeV has revived the interest in supersymmetric models, which predicted a Higgs boson mass below 130 GeV long before its discovery. We compare systematically the…

High Energy Physics - Phenomenology · Physics 2015-06-16 C. Beskidt , W. de Boer , D. I. Kazakov

If the Higgs boson has a mass below 130 GeV, then the standard model vacuum is unstable; if it has a mass below 90 GeV (i.e. within reach of LEP within the next two years), then the instability will occur at a scale between 800 GeV and 10…

High Energy Physics - Phenomenology · Physics 2015-06-25 P. Q. Hung , Marc Sher

Supersymmetric models with an additional singlet field offer the Higgs boson the possibility to decay to two pseudoscalars, a. If the mass of these pseudoscalars is above the b bbar threshold, a -> b bbar is generically the dominant decay…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tim Stelzer , Soren Wiesenfeldt , Scott Willenbrock

A search is performed for a Higgs boson produced in association with a Z boson and decaying into two photons, using the L3 data collected at LEP at a centre-of-mass energy of 189 GeV. All decay modes of the Z are considered. No signal is…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

In light of current atmospheric neutrino oscillation data, we revisit the invisible decay of the standard model Higgs boson and other pseudoscalar mesons which can be enhanced because of large number of KK modes in models with right handed…

High Energy Physics - Phenomenology · Physics 2009-11-10 N. G. Deshpande , Dilip Kumar Ghosh

The dominance of $h\to \eta \eta$ decay mode for the intermediate mass Higgs boson is highly motivated to solve the little hierarchy problem and to ease the tension with the precision data. However, the discovery modes for $m_h \alt 150$…

High Energy Physics - Phenomenology · Physics 2007-10-11 Kingman Cheung , Jeonghyeon Song , Qi-Shu Yan

We review the present status of Higgs physics within the standard model and its extensions. First, we briefly summarize the current experimental exclusion limits from the direct searches with LEP1 and the Tevatron, and assess the discovery…

High Energy Physics - Phenomenology · Physics 2007-05-23 Bernd A. Kniehl

We consider the possibility that the heavier CP-even Higgs boson~($H^0$) in the minimal supersymmetric standard model (MSSM) decays invisibly into neutralinos in the light of the recent discovery of the 126 GeV resonance at the CERN Large…

High Energy Physics - Phenomenology · Physics 2015-07-15 B. Ananthanarayan , Jayita Lahiri , P. N. Pandita

We examine the parameter space of the purely phenomenological minimal super- symmetric standard model (MSSM), without assuming any supersymmetry breaking scheme. We find that a large region of the parameter space can indeed yield the…

High Energy Physics - Phenomenology · Physics 2012-02-29 Nishita Desai , Biswarup Mukhopadhyaya , Saurabh Niyogi