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We show that the gauge mediation models with vector-like matters can explain the Higgs boson mass of 126 GeV without large soft scalar masses nor a large left-right mixing of the stops. The scenario has interesting features: the existence…

High Energy Physics - Phenomenology · Physics 2013-05-09 Norimi Yokozaki

In a simplified version of the standard model with a single quark doublet, I derive a transcendental equation for the complex Higgs boson mass. The equation involves a divergent integral which is regularized and renormalized conventionally.…

High Energy Physics - Phenomenology · Physics 2024-07-16 Gregory A. Wright

We obtain the bounds on all the gauge invariant, flavour symmetric, CP-even operators of dimension 6 that can affect the electroweak precision tests. For the preferred Higgs mass of about 100 GeV, their minimal scales range from 2 to 10…

High Energy Physics - Phenomenology · Physics 2009-10-09 Riccardo Barbieri , Alessandro Strumia

We discuss the possibility of interpreting the 125 GeV scalar boson and the 750 GeV diphoton excess recently reported by the ATLAS and CMS experiments as a Higgs-dominated and a radion-dominated states respectively in a stabilized…

High Energy Physics - Phenomenology · Physics 2016-05-30 Edward E. Boos , Viacheslav E. Bunichev , Igor P. Volobuev

In this paper, we study two Higgs doublet models with gauged U(1)_H symmetry, motivated by the excesses around 96 GeV reported by the CMS collaboration in the searches for light resonances decaying to two photons and two \tau's. In this…

High Energy Physics - Phenomenology · Physics 2025-08-29 Seungwon Baek , P. Ko , Yuji Omura , Chaehyun Yu

If the Higgs boson indeed weighs about 114 to 115 GeV, there must be new physics beyond the Standard Model at some scale \la 10^6 GeV. The most plausible new physics is supersymmetry, which predicts a Higgs boson weighing \la 130 GeV. In…

High Energy Physics - Phenomenology · Physics 2009-09-11 J. Ellis , G. Ganis , D. V. Nanopoulos , K. A. Olive

The Large Volume Scenario for getting a non-supersymmetric vacuum in type IIB string theory leads, through the Weyl anomaly and renormalization group running, to an interesting phenomenology. However, for gravitino masses below 500 TeV…

High Energy Physics - Phenomenology · Physics 2015-06-04 Senarath de Alwis , Kevin Givens

A search for a narrow Higgs boson resonance in the diphoton mass spectrum is presented based on data corresponding to 7.0 fb^-1 of integrated luminosity from p-pbar collisions at sqrt(s) = 1.96 TeV collected by the CDF experiment. No…

High Energy Physics - Experiment · Physics 2015-05-30 CDF Collaboration , T. Aaltonen , B. Alvarez Gonzalez , S. Amerio , D. Amidei , A. Anastassov , A. Annovi , J. Antos , G. Apollinari , J. A. Appel , A. Apresyan , T. Arisawa , A. Artikov , J. Asaadi , W. Ashmanskas , B. Auerbach , A. Aurisano , F. Azfar , W. Badgett , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barria , P. Bartos , M. Bauce , G. Bauer , F. Bedeschi , D. Beecher , S. Behari , G. Bellettini , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , M. Binkley , D. Bisello , I. Bizjak , K. R. Bland , B. Blumenfeld , A. Bocci , A. Bodek , D. Bortoletto , J. Boudreau , A. Boveia , L. Brigliadori , A. Brisuda , C. Bromberg , E. Brucken , M. Bucciantonio , J. Budagov , H. S. Budd , S. Budd , K. Burkett , G. Busetto , P. Bussey , A. Buzatu , C. Calancha , S. Camarda , M. Campanelli , M. Campbell , F. Canelli , B. Carls , D. Carlsmith , R. Carosi , S. Carrillo , S. Carron , B. Casal , M. Casarsa , A. Castro , P. Catastini , D. Cauz , V. Cavaliere , M. Cavalli-Sforza , A. Cerri , L. Cerrito , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , J. P. Chou , W. H. Chung , Y. S. Chung , C. I. Ciobanu , M. A. Ciocci , A. Clark , C. Clarke , G. Compostella , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Crescioli , C. Cuenca Almenar , J. Cuevas , R. Culbertson , D. Dagenhart , N. d'Ascenzo , M. Datta , P. de Barbaro , S. De Cecco , G. De Lorenzo , M. Dell'Orso , C. Deluca , L. Demortier , J. Deng , M. Deninno , F. Devoto , M. d'Errico , A. Di Canto , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donati , P. Dong , M. Dorigo , T. Dorigo , K. Ebina , A. Elagin , A. Eppig , R. Erbacher , D. Errede , S. Errede , N. Ershaidat , R. Eusebi , H. C. Fang , S. Farrington , M. Feindt , J. P. Fernandez , C. Ferrazza , R. Field , G. Flanagan , R. Forrest , M. J. Frank , M. Franklin , J. C. Freeman , Y. Funakoshi , I. Furic , M. Gallinaro , J. Galyardt , J. E. Garcia , A. F. Garfinkel , P. Garosi , H. Gerberich , E. Gerchtein , S. Giagu , V. Giakoumopoulou , P. Giannetti , K. Gibson , C. M. Ginsburg , N. Giokaris , P. Giromini , M. Giunta , G. Giurgiu , V. Glagolev , D. Glenzinski , M. Gold , D. Goldin , N. Goldschmidt , A. Golossanov , G. Gomez , G. Gomez-Ceballos , M. Goncharov , O. Gonzalez , I. Gorelov , A. T. Goshaw , K. Goulianos , S. Grinstein , C. Grosso-Pilcher , R. C. Group , J. Guimaraes da Costa , Z. Gunay-Unalan , C. Haber , S. R. Hahn , E. Halkiadakis , A. Hamaguchi , J. Y. Han , F. Happacher , K. Hara , D. Hare , M. Hare , R. F. Harr , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , S. Hewamanage , D. Hidas , A. Hocker , W. Hopkins , D. Horn , S. Hou , R. E. Hughes , M. Hurwitz , U. Husemann , N. Hussain , M. Hussein , J. Huston , G. Introzzi , M. Iori , A. Ivanov , E. James , D. Jang , B. Jayatilaka , E. J. Jeon , M. K. Jha , S. Jindariani , W. Johnson , M. Jones , K. K. Joo , S. Y. Jun , T. R. Junk , T. Kamon , P. E. Karchin , A. Kasmi , Y. Kato , W. Ketchum , J. Keung , V. Khotilovich , B. Kilminster , D. H. Kim , H. S. Kim , H. W. Kim , J. E. Kim , M. J. Kim , S. B. Kim , S. H. Kim , Y. K. Kim , N. Kimura , M. Kirby , S. Klimenko , K. Kondo , D. J. Kong , J. Konigsberg , A. V. Kotwal , M. Kreps , J. Kroll , D. Krop , N. Krumnack , M. Kruse , V. Krutelyov , T. Kuhr , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannon , A. Lath , G. Latino , T. LeCompte , E. Lee , H. S. Lee , J. S. Lee , S. W. Lee , S. Leo , S. Leone , J. D. Lewis , A. Limosani , C. -J. Lin , J. Linacre , M. Lindgren , E. Lipeles , A. Lister , D. O. Litvintsev , C. Liu , Q. Liu , T. Liu , S. Lockwitz , A. Loginov , D. Lucchesi , J. Lueck , P. Lujan , P. Lukens , G. Lungu , J. Lys , R. Lysak , R. Madrak , K. Maeshima , K. Makhoul , S. Malik , G. Manca , A. Manousakis-Katsikakis , F. Margaroli , C. Marino , M. Martinez , R. Martinez-Ballarin , P. Mastrandrea , M. E. Mattson , P. Mazzanti , K. S. McFarland , P. McIntyre , R. McNulty , A. Mehta , P. Mehtala , A. Menzione , C. Mesropian , T. Miao , D. Mietlicki , A. Mitra , H. Miyake , S. Moed , N. Moggi , M. N. Mondragon , C. S. Moon , R. Moore , M. J. Morello , J. Morlock , P. Movilla Fernandez , A. Mukherjee , Th. Muller , P. Murat , M. Mussini , J. Nachtman , Y. Nagai , J. Naganoma , I. Nakano , A. Napier , J. Nett , C. Neu , M. S. Neubauer , J. Nielsen , L. Nodulman , O. Norniella , E. Nurse , L. Oakes , S. H. Oh , Y. D. Oh , I. Oksuzian , T. Okusawa , R. Orava , L. Ortolan , S. Pagan Griso , C. Pagliarone , E. Palencia , V. Papadimitriou , A. A. Paramonov , J. Patrick , G. Pauletta , M. Paulini , C. Paus , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , J. Pilot , K. Pitts , C. Plager , L. Pondrom , S. Poprocki , K. Potamianos , O. Poukhov , F. Prokoshin , A. Pronko , F. Ptohos , E. Pueschel , G. Punzi , J. Pursley , A. Rahaman , V. Ramakrishnan , N. Ranjan , J. Ray , I. Redondo , P. Renton , M. Rescigno , T. Riddick , F. Rimondi , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rolli , R. Roser , M. Rossi , F. Rubbo , F. Ruffini , A. Ruiz , J. Russ , V. Rusu , A. Safonov , W. K. Sakumoto , Y. Sakurai , L. Santi , L. Sartori , K. Sato , V. Saveliev , A. Savoy-Navarro , P. Schlabach , A. Schmidt , E. E. Schmidt , M. P. Schmidt , M. Schmitt , T. Schwarz , L. Scodellaro , A. Scribano , F. Scuri , A. Sedov , S. Seidel , Y. Seiya , A. Semenov , F. Sforza , A. Sfyrla , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojima , S. Shiraishi , M. Shochet , I. Shreyber , A. Simonenko , P. Sinervo , A. Sissakian , K. Sliwa , J. R. Smith , F. D. Snider , A. Soha , S. Somalwar , V. Sorin , P. Squillacioti , M. Stancari , M. Stanitzki , R. St. Denis , B. Stelzer , O. Stelzer-Chilton , D. Stentz , J. Strologas , G. L. Strycker , Y. Sudo , A. Sukhanov , I. Suslov , K. Takemasa , Y. Takeuchi , J. Tang , M. Tecchio , P. K. Teng , J. Thom , J. Thome , G. A. Thompson , E. Thomson , P. Ttito-Guzman , S. Tkaczyk , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totaro , M. Trovato , Y. Tu , F. Ukegawa , S. Uozumi , A. Varganov , F. Vazquez , G. Velev , C. Vellidis , M. Vidal , I. Vila , R. Vilar , J. Vizan , M. Vogel , G. Volpi , P. Wagner , R. L. Wagner , T. Wakisaka , R. Wallny , S. M. Wang , A. Warburton , D. Waters , M. Weinberger , W. C. Wester , B. Whitehouse , D. Whiteson , A. B. Wicklund , E. Wicklund , S. Wilbur , F. Wick , H. H. Williams , J. S. Wilson , P. Wilson , B. L. Winer , P. Wittich , S. Wolbers , H. Wolfe , T. Wright , X. Wu , Z. Wu , K. Yamamoto , J. Yamaoka , T. Yang , U. K. Yang , Y. C. Yang , W. -M. Yao , G. P. Yeh , K. Yi , J. Yoh , K. Yorita , T. Yoshida , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , S. Zucchelli

The BMSSM framework is an effective theory approach that encapsulates a variety of extensions beyond the MSSM with which it shares the same field content. The lightest Higgs mass can be much heavier than in the MSSM without creating a…

High Energy Physics - Phenomenology · Physics 2015-06-04 Fawzi Boudjema , Guillaume Drieu La Rochelle

The allowed standard model Higgs mass range has been reduced to a region between 114 and 130 GeV or above 500 GeV, at the 99% confidence level, since the Large Hadron Collider (LHC) program started. Furthermore some of the experiments at…

High Energy Physics - Phenomenology · Physics 2012-03-20 Mads T. Frandsen , Francesco Sannino

We propose a simple gauge extension of the minimal supersymmetric standard model (MSSM), where the fine tuning in the Higgs mass parameters is highly reduced. The Higgs boson is insensitive to high energies because of supersymmetry and also…

High Energy Physics - Phenomenology · Physics 2010-04-15 B. Bellazzini , C. Csaki , A. Delgado , A. Weiler

We construct a general class of pseudo-Goldstone composite Higgs models, within the minimal SO(5)/SO(4) coset structure, that are not necessarily of moose-type. We characterize the main properties these models should have in order to give…

High Energy Physics - Phenomenology · Physics 2015-06-05 David Marzocca , Marco Serone , Jing Shu

In the Standard Model (SM), the weak gauge bosons and fermions acquire mass through the Higgs mechanism. A lower limit on the SM Higgs mass of 114.4 GeV was obtained from the direct search at LEP. Although a single Higgs doublet is…

High Energy Physics - Experiment · Physics 2007-05-23 Andre G. Holzner

A Higgs particle produced in association with a Z boson and decaying into two photons is searched for in the data collected by the L3 experiment at LEP. All possible decay modes of the Z boson are investigated. No signal is observed in…

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

The Higgs boson, a fundamental scalar, was discovered at CERN in 2012 with mass 125 GeV, a mass that turned out to be a remarkable choice of Nature. In the Standard Model of particle physics, the Higgs boson is closely linked to the…

High Energy Physics - Phenomenology · Physics 2021-09-06 Steven D. Bass , Albert De Roeck , Marumi Kado

I discuss standard motivation for the new physics at the 1 TeV scale. Although the arguments for new exotic phenomena seem to be very supportive I argue that the Standard Model still might offer a good description far beyond this energy…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marko B. Popovic

It is noticed that the total relative density of mass in the Universe Omega_tot should exceed 1, i.e. Omega_tot=1+f^2/6 according to the field relativistic theory of gravity (RTG), which is free of the cosmological singularity and which…

Astrophysics · Physics 2009-11-07 S. S. Gershtein , A. A. Logunov , M. A. Mestvirishvili

Naturalness has for many years been a guiding principle in the search for physics beyond the Standard Model, particularly for understanding the physics of electroweak symmetry breaking. However, the discovery of the Higgs particle at 125…

High Energy Physics - Phenomenology · Physics 2015-01-12 Michael Dine

The properties of 125 GeV new particle, which was discovered in 2012 at the Large Hadron Collider (LHC), are found to be consistent with those of the Higgs boson in the standard model (SM). Hereafter the new particle is dubbed as SM-like…

High Energy Physics - Phenomenology · Physics 2014-05-12 Xiao-ping Wang , Shou-hua Zhu

The discovery of the Higgs boson at the LHC, and especially the determination of its mass around 125 GeV, together with the absence of any trace of new physics make it conceivable that we live in a metastable (but long-lived) electroweak…

High Energy Physics - Lattice · Physics 2013-11-11 Jose R. Espinosa
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