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Related papers: Exploring Dimuon Higgs Decay in an Extended Scotog…

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We investigate the extended Higgs sectors, specially the charged Higgs sector in a supersymmetric $Y=0$ $SU(2)$ triplet and a Standard Model (SM) gauge singlet extension of SM. We show that in this model the allowed data for the Higgs boson…

High Energy Physics - Phenomenology · Physics 2016-10-05 Priyotosh Bandyopadhyay , Claudio Coriano , Antonio Costantini

The Next-to-Minimal Supersymmetric Standard Model (NMSSM) offers a rich framework embedding physics beyond the Standard Model as well as consistent interpretations of the results about the Higgs signal detected at the LHC. We investigate…

High Energy Physics - Phenomenology · Physics 2018-12-05 Florian Domingo , Sven Heinemeyer , Sebastian Paßehr , Georg Weiglein

We study the electroweak phase transition and the critical bubble in the scale-invariant two Higgs doublet model taking the recent LHC data into account. The sphaleron energy in this model is evaluated for the first time. It is found that…

High Energy Physics - Phenomenology · Physics 2015-05-22 Kaori Fuyuto , Eibun Senaha

A search for the dimuon decay of the Standard Model (SM) Higgs boson is performed using data corresponding to an integrated luminosity of 139 fb$^{-1}$ collected with the ATLAS detector in Run2 $pp$ collisions at $\sqrt{s}=13$ TeV at the…

High Energy Physics - Experiment · Physics 2020-12-18 ATLAS Collaboration

We studied the extension of Standard Model (SM) Higgs sector with $SU(2)$ triplet and SM gauge singlet in the context of supersymmetry. For a $Z_3$ symmetric superpotential where the singlet field generates the bi-linear Higgs mixing term…

High Energy Physics - Phenomenology · Physics 2016-12-21 Priyotosh Bandyopadhyay

We consider implications of the diphoton excess recently observed at the LHC on the anomalous magnetic dipole moment of the muon $(g-2)_\mu = 2 a_\mu$, hypothesizing that the possible 750 GeV resonance is a (pseudo)scalar particle. The…

High Energy Physics - Phenomenology · Physics 2016-05-20 Seungwon Baek , Jae-hyeon Park

We consider next-to-minimal supersymmetric standard model (NMSSM) which has a gauge singlet superfield. In the scale invariant superpotential we do not have the mass terms and the whole Lagrangian has an additional $Z_3$ symmetry. This…

High Energy Physics - Phenomenology · Physics 2016-07-12 Priyotosh Bandyopadhyay , Katri Huitu , Saurabh Niyogi

One loop corrections to the muon decay are studied in a popular and self-consistent version of the Left-Right symmetric model. It is shown quantitatively, that the corrections do not split into those that come from the Standard Model sector…

High Energy Physics - Phenomenology · Physics 2011-01-13 M. Czakon , J. Gluza , J. Hejczyk

Discovery of the Higgs boson decay to dimuon is anticipated soon based on the current evidence. Precise categorization of the events without affecting the invariant mass shape is crucial in the analysis. Decorrelation of the invariant mass…

High Energy Physics - Phenomenology · Physics 2024-10-21 Subin Han , Hyung Do Kim

We study the decay of the metastable symmetric phase in the standard model at finite temperature. For the SU(2)-Higgs model the two wave function correction terms $Z_{\vp}(\vp^2,T)$ and $Z_{\chi}(\vp^2,T)$ of Higgs and Goldstone boson…

High Energy Physics - Phenomenology · Physics 2009-10-22 D. Bödeker , W. Buchmüller , Z. Fodor , T. Helbig

In this work, we present a scotogenic model, where the neutrino mass is generated at one-loop diagrams. The standard model (SM) is extended by three singlet Majorana fermions and two inert scalar doublets instead of one doublet as in the…

High Energy Physics - Phenomenology · Physics 2023-02-07 Amine Ahriche

The angular distributions and the partial branching fraction of the decay $B^{0} \rightarrow K^{*0} \mu^+ \mu^-$ are studied using an integrated luminosity of $0.37\,fb^{-1}$ of data collected with the LHCb detector. The forward-backward…

High Energy Physics - Experiment · Physics 2012-05-17 LHCb Collaboration , R. Aaij , C. Abellan Beteta , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , Y. Amhis , J. Anderson , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , L. Arrabito , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , S. Bachmann , J. J. Back , D. S. Bailey , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , A. Bates , C. Bauer , Th. Bauer , A. Bay , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , M. Benayoun , G. Bencivenni , S. Benson , J. Benton , R. Bernet , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , C. Blanks , J. Blouw , S. Blusk , A. Bobrov , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , T. J. V. Bowcock , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , D. Brett , M. Britsch , T. Britton , N. H. Brook , H. Brown , A. Büchler-Germann , I. Burducea , A. Bursche , J. Buytaert , S. Cadeddu , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , P. Campana , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , L. Carson , K. Carvalho Akiba , G. Casse , M. Cattaneo , Ch. Cauet , M. Charles , Ph. Charpentier , N. Chiapolini , K. Ciba , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , P. Collins , A. Comerma-Montells , F. Constantin , A. Contu , A. Cook , M. Coombes , G. Corti , G. A. Cowan , R. Currie , C. D'Ambrosio , P. David , P. N. Y. David , I. De Bonis , S. De Capua , M. De Cian , F. De Lorenzi , J. M. De Miranda , L. De Paula , P. De Simone , D. Decamp , M. Deckenhoff , H. Degaudenzi , L. Del Buono , C. Deplano , D. Derkach , O. Deschamps , F. Dettori , J. Dickens , H. Dijkstra , P. Diniz Batista , F. Domingo Bonal , S. Donleavy , F. Dordei , A. Dosil Suárez , D. Dossett , A. Dovbnya , F. Dupertuis , R. Dzhelyadin , A. Dziurda , S. Easo , U. Egede , V. Egorychev , S. Eidelman , D. van Eijk , F. Eisele , S. Eisenhardt , R. Ekelhof , L. Eklund , Ch. Elsasser , D. Elsby , D. Esperante Pereira , L. Estève , A. Falabella , E. Fanchini , C. Färber , G. Fardell , C. Farinelli , S. Farry , V. Fave , V. Fernandez Albor , M. Ferro-Luzzi , S. Filippov , C. Fitzpatrick , M. Fontana , F. Fontanelli , R. Forty , M. Frank , C. Frei , M. Frosini , S. Furcas , A. Gallas Torreira , D. Galli , M. Gandelman , P. Gandini , Y. Gao , J-C. Garnier , J. Garofoli , J. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , N. Gauvin , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , H. Gordon , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , E. Greening , S. Gregson , B. Gui , E. Gushchin , Yu. Guz , T. Gys , G. Haefeli , C. Haen , S. C. Haines , T. Hampson , S. Hansmann-Menzemer , R. Harji , N. Harnew , J. Harrison , P. F. Harrison , T. Hartmann , J. He , V. Heijne , K. Hennessy , P. Henrard , J. A. Hernando Morata , E. van Herwijnen , E. Hicks , K. Holubyev , P. Hopchev , W. Hulsbergen , P. Hunt , T. Huse , R. S. Huston , D. Hutchcroft , D. Hynds , V. Iakovenko , P. Ilten , J. Imong , R. Jacobsson , A. Jaeger , M. Jahjah Hussein , E. Jans , F. Jansen , P. Jaton , B. Jean-Marie , F. Jing , M. John , D. Johnson , C. R. Jones , B. Jost , M. Kaballo , S. Kandybei , M. Karacson , T. M. Karbach , J. Keaveney , I. R. Kenyon , U. Kerzel , T. Ketel , A. Keune , B. Khanji , Y. M. Kim , M. Knecht , P. Koppenburg , A. Kozlinskiy , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , K. Kruzelecki , M. Kucharczyk , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , E. Lanciotti , G. Lanfranchi , C. Langenbruch , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , O. Leroy , T. Lesiak , L. Li , L. Li Gioi , M. Lieng , M. Liles , R. Lindner , C. Linn , B. Liu , G. Liu , J. von Loeben , J. H. Lopes , E. Lopez Asamar , N. Lopez-March , H. Lu , J. Luisier , A. Mac Raighne , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , J. Magnin , S. Malde , R. M. D. Mamunur , G. Manca , G. Mancinelli , N. Mangiafave , U. Marconi , R. Märki , J. Marks , G. Martellotti , A. Martens , L. Martin , A. Martín Sánchez , D. Martinez Santos , A. Massafferri , Z. Mathe , C. Matteuzzi , M. Matveev , E. Maurice , B. Maynard , A. Mazurov , G. McGregor , R. McNulty , M. Meissner , M. Merk , J. Merkel , R. Messi , S. Miglioranzi , D. A. Milanes , M. -N. Minard , J. Molina Rodriguez , S. Monteil , D. Moran , P. Morawski , R. Mountain , I. Mous , F. Muheim , K. Müller , R. Muresan , B. Muryn , B. Muster , M. Musy , J. Mylroie-Smith , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Nedos , M. Needham , N. Neufeld , C. Nguyen-Mau , M. Nicol , V. Niess , N. Nikitin , A. Nomerotski , A. Novoselov , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , M. Orlandea , J. M. Otalora Goicochea , P. Owen , K. Pal , J. Palacios , A. Palano , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , S. K. Paterson , G. N. Patrick , C. Patrignani , C. Pavel-Nicorescu , A. Pazos Alvarez , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , D. L. Perego , E. Perez Trigo , A. Pérez-Calero Yzquierdo , P. Perret , M. Perrin-Terrin , G. Pessina , A. Petrella , A. Petrolini , A. Phan , E. Picatoste Olloqui , B. Pie Valls , B. Pietrzyk , T. Pilař , D. Pinci , R. Plackett , S. Playfer , M. Plo Casasus , G. Polok , A. Poluektov , E. Polycarpo , D. Popov , B. Popovici , C. Potterat , A. Powell , J. Prisciandaro , V. Pugatch , A. Puig Navarro , W. Qian , J. H. Rademacker , B. Rakotomiaramanana , M. S. Rangel , I. Raniuk , G. Raven , S. Redford , M. M. Reid , A. C. dos Reis , S. Ricciardi , K. Rinnert , D. A. Roa Romero , P. Robbe , E. Rodrigues , F. Rodrigues , P. Rodriguez Perez , G. J. Rogers , S. Roiser , V. Romanovsky , M. Rosello , J. Rouvinet , T. Ruf , H. Ruiz , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , C. Salzmann , M. Sannino , R. Santacesaria , C. Santamarina Rios , R. Santinelli , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Savrie , D. Savrina , P. Schaack , M. Schiller , S. Schleich , M. Schlupp , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , M. Seco , A. Semennikov , K. Senderowska , I. Sepp , N. Serra , J. Serrano , P. Seyfert , M. Shapkin , I. Shapoval , P. Shatalov , Y. Shcheglov , T. Shears , L. Shekhtman , O. Shevchenko , V. Shevchenko , A. Shires , R. Silva Coutinho , T. Skwarnicki , A. C. Smith , N. A. Smith , E. Smith , K. Sobczak , F. J. P. Soler , A. Solomin , F. Soomro , B. Souza De Paula , B. Spaan , A. Sparkes , P. Spradlin , F. Stagni , S. Stahl , O. Steinkamp , S. Stoica , S. Stone , B. Storaci , M. Straticiuc , U. Straumann , V. K. Subbiah , S. Swientek , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , E. Teodorescu , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Topp-Joergensen , N. Torr , E. Tournefier , M. T. Tran , A. Tsaregorodtsev , N. Tuning , M. Ubeda Garcia , A. Ukleja , P. Urquijo , U. Uwer , V. Vagnoni , G. Valenti , R. Vazquez Gomez , P. Vazquez Regueiro , S. Vecchi , J. J. Velthuis , M. Veltri , B. Viaud , I. Videau , X. Vilasis-Cardona , J. Visniakov , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , H. Voss , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , A. D. Webber , D. Websdale , M. Whitehead , D. Wiedner , L. Wiggers , G. Wilkinson , M. P. Williams , M. Williams , F. F. Wilson , J. Wishahi , M. Witek , W. Witzeling , S. A. Wotton , K. Wyllie , Y. Xie , F. Xing , Z. Xing , Z. Yang , R. Young , O. Yushchenko , M. Zavertyaev , F. Zhang , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , L. Zhong , E. Zverev , A. Zvyagin

We revisit the rare decays of the Higgs boson to two different quarks in the Standard Model, which arise at the one-loop level. We perform Taylor series expansions to the complete form factors of the decay amplitudes, according to their…

High Energy Physics - Phenomenology · Physics 2020-12-02 J. I. Aranda , G. González-Estrada , J. Montaño , F. Ramírez-Zavaleta , E. S. Tututi

Beyond the Standard Model (SM) extensions usually include extended Higgs sectors. Models with singlet or doublet fields are the simplest ones that are compatible with the $\rho$ parameter constraint. The discovery of new non-SM Higgs bosons…

High Energy Physics - Phenomenology · Physics 2017-10-04 M. Muhlleitner , M. Sampaio , R. Santos , J. Wittbrodt

We study the observability of the $h\to \mu^+\mu^-$ decay in the Standard Model and the MSSM at the LHC. The observation of the $h\mu\mu$ coupling is important to determine whether the Higgs particle that generates mass for the weak bosons…

High Energy Physics - Phenomenology · Physics 2009-11-07 Tao Han , Bob McElrath

We consider isosinglet scalar extension of a model with a Higgs democracy - multihiggs extension of the SM where each quark and lepton has its own Higgs isodoublet. The addition of light isosinglet scalar allows to solve both muon…

High Energy Physics - Phenomenology · Physics 2017-10-18 N. V. Krasnikov

Motivated by the LHCb measurement of the hyperon decay mode $\Sigma^+\to p\mu^+\mu^-$ and prospects for improvement, we revisit the estimates for the rate and muon forward-backward asymmetry within the standard model and beyond. The…

High Energy Physics - Phenomenology · Physics 2025-01-16 Arnab Roy , Jusak Tandean , German Valencia

We examine the leptophilic two Higgs doublet model with fermionic dark matter, considering the range of experimental constraints on the Higgs sector. The measurements of the 125 GeV Higgs from the LHC Run-I allow us to focus on those…

High Energy Physics - Phenomenology · Physics 2015-10-28 Matthew R. Buckley , David Feld

Higgs sectors extended by electroweakly charged scalars can be explored by scalar pair production at the LHC. We consider a fermiophobic scenario, with decays into a pair of gauge bosons, and a fermiophilic one, with decays into top and…

High Energy Physics - Phenomenology · Physics 2023-01-04 G. Cacciapaglia , T. Flacke , M. Kunkel , W. Porod , L. Schwarze

We show that the recent discovery of a new boson at the LHC, which we assume to be a Higgs boson, and the observed enhancement in its diphoton decays compared to the SM prediction, can be explained by a new doublet of charged vector bosons…

High Energy Physics - Phenomenology · Physics 2015-06-05 Alexandre Alves , A. G. Dias , E. Ramirez Barreto , C. A. de S. Pires , Farinaldo S. Queiroz , P. S. Rodrigues da Silva