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We consider the generation of the baryon asymmetry in the two-Higgs doublet model. Investigating the thermal potential in the presence of CP violation, as relevant for baryogenesis, we find a strong first-order phase transition if the extra…

High Energy Physics - Phenomenology · Physics 2011-09-29 Lars Fromme , Stephan J. Huber , Michael Seniuch

If the Higgs boson weighs about 115 GeV, the effective potential of the Standard Model becomes unstable above a scale of about 10^6 GeV. This instability may be rectified only by new bosonic particles such as stop squarks. However, avoiding…

High Energy Physics - Phenomenology · Physics 2009-09-11 John Ellis , Douglas Ross

Depending on the Higgs-boson and top-quark masses, $M_H$ and $M_t$, the effective potential of the {\bf Standard Model} can develop a non-standard minimum for values of the field much larger than the weak scale. In those cases the standard…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Quirós

Results are reported from a search for non-standard-model Higgs boson decays to pairs of new light bosons, each of which decays into the oppositely charged dimuon final state. The new bosons may be produced either promptly or via a decay…

High Energy Physics - Experiment · Physics 2013-11-11 CMS Collaboration

Preliminary results of the search for a Standard Model like Higgs boson at the LHC with 5 fb-1 data have just been presented by the ATLAS and CMS collaborations and an excess of events at a mass of ~125 GeV has been reported. If this excess…

High Energy Physics - Phenomenology · Physics 2012-01-26 A. Arbey , M. Battaglia , A. Djouadi , F. Mahmoudi , J. Quevillon

A search is presented for a heavy pseudoscalar boson A decaying to a Z boson and a Higgs boson with mass of 125 GeV. In the final state considered, the Higgs boson decays to a bottom quark and antiquark, and the Z boson decays either into a…

High Energy Physics - Experiment · Physics 2019-07-10 CMS Collaboration

The discovery of the long awaited Higgs boson is described using data from the CMS detector at the LHC. In the SM the masses of fermions and the heavy gauge bosons are generated by the interactions with the Higgs field, so all couplings are…

High Energy Physics - Phenomenology · Physics 2013-09-04 W. de Boer

We show that there are regions in the parameter space of the Littlest Higgs model with T-parity, allowed by electroweak precision data, where the Higgs boson can decay invisibly into a pair of heavy photons A_H with a substantial branching…

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

With no conclusive signal till date of the minimal supersymmetric and extra dimensional models at the Large Hadron Collider (LHC), the issue of fine-tuning of the Higgs mass still calls for some attention. It could be very possible that the…

High Energy Physics - Phenomenology · Physics 2019-03-27 Nabarun Chakrabarty , Indrani Chakraborty

A new particle - discovered recently with the Atlas and CMS detectors at LHC - has been interpreted as the long sought Higgs-boson. A corresponding scalar field is needed to make the weak interaction gauge invariant and to understand the…

General Physics · Physics 2013-10-01 H. P. Morsch

The generation of the baryon asymmetry of the universe is considered in the standard model of the electroweak theory with simple extensions of the Higgs sector. The propagation of quarks of masses up to about 5 GeV are considered, taking…

High Energy Physics - Phenomenology · Physics 2010-11-01 A. Kundu , S. Mallik

In the unified subquark model of all fundamental particles and forces, the mass of the Higgs boson in the standard model of electroweak interactions ($m_H$) is predicted to be about $2\sqrt{6}m_W/3$ (where $m_W$ is the mass of the charged…

High Energy Physics - Phenomenology · Physics 2015-06-18 Hidezumi Terazawa , Masaki Yasue

A search is presented for massive long-lived particles, in the 20-60 GeV mass range with lifetimes between 5 and 100 ps. The dataset used corresponds to 0.62 1\fb of proton-proton collision data collected by the LHCb detector at sqrt(s)=7…

High Energy Physics - Experiment · Physics 2018-11-22 LHCb collaboration , R. Aaij , B. Adeva , M. Adinolfi , Z. Ajaltouni , S. Akar , J. Albrecht , F. Alessio , M. Alexander , S. Ali , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , S. Amerio , Y. Amhis , L. An , L. Anderlini , G. Andreassi , M. Andreotti , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , P. d'Argent , J. Arnau Romeu , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , M. Baalouch , S. Bachmann , J. J. Back , A. Badalov , C. Baesso , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , V. Batozskaya , V. Battista , A. Bay , L. Beaucourt , J. Beddow , F. Bedeschi , I. Bediaga , L. J. Bel , V. Bellee , N. Belloli , K. Belous , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , A. Bertolin , M. -O. Bettler , M. van Beuzekom , I. Bezshyiko , S. Bifani , P. Billoir , T. Bird , A. Birnkraut , A. Bitadze , A. Bizzeti , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , T. Boettcher , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , M. Borisyak , M. Borsato , F. Bossu , M. Boubdir , T. J. V. Bowcock , E. Bowen , C. Bozzi , S. Braun , M. Britsch , T. Britton , J. Brodzicka , E. Buchanan , C. Burr , A. Bursche , J. Buytaert , S. Cadeddu , R. Calabrese , M. Calvi , M. Calvo Gomez , P. Campana , D. Campora Perez , L. Capriotti , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , P. Carniti , L. Carson , K. Carvalho Akiba , G. Casse , L. Cassina , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , G. Cavallero , R. Cenci , M. Charles , Ph. Charpentier , G. Chatzikonstantinidis , M. Chefdeville , S. Chen , S. -F. Cheung , V. Chobanova , M. Chrzaszcz , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , V. Coco , J. Cogan , E. Cogneras , V. Cogoni , L. Cojocariu , G. Collazuol , P. Collins , A. Comerma-Montells , A. Contu , A. Cook , S. Coquereau , G. Corti , M. Corvo , C. M. Costa Sobral , B. Couturier , G. A. Cowan , D. C. Craik , A. Crocombe , M. Cruz Torres , S. Cunliffe , R. Currie , C. D'Ambrosio , E. Dall'Occo , J. Dalseno , P. N. Y. David , A. Davis , O. De Aguiar Francisco , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , P. De Simone , C. -T. Dean , D. Decamp , M. Deckenhoff , L. Del Buono , M. Demmer , D. Derkach , O. Deschamps , F. Dettori , B. Dey , A. Di Canto , H. Dijkstra , F. Dordei , M. Dorigo , A. Dosil Suárez , A. Dovbnya , K. Dreimanis , L. Dufour , G. Dujany , K. Dungs , P. Durante , R. Dzhelyadin , A. Dziurda , A. Dzyuba , N. Déléage , S. Easo , U. Egede , V. Egorychev , S. Eidelman , S. Eisenhardt , U. Eitschberger , R. Ekelhof , L. Eklund , Ch. Elsasser , S. Ely , S. Esen , H. M. Evans , T. Evans , A. Falabella , N. Farley , S. Farry , R. Fay , D. Ferguson , V. Fernandez Albor , F. Ferrari , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , M. Fiorini , M. Firlej , C. Fitzpatrick , T. Fiutowski , F. Fleuret , K. Fohl , M. Fontana , F. Fontanelli , D. C. Forshaw , R. Forty , M. Frank , C. Frei , M. Frosini , J. Fu , E. Furfaro , C. Färber , A. Gallas Torreira , D. Galli , S. Gallorini , S. Gambetta , M. Gandelman , P. Gandini , Y. Gao , J. García Pardiñas , J. Garra Tico , L. Garrido , P. J. Garsed , D. Gascon , C. Gaspar , L. Gavardi , G. Gazzoni , D. Gerick , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , S. Gianì , V. Gibson , O. G. Girard , L. Giubega , K. Gizdov , V. V. Gligorov , D. Golubkov , A. Golutvin , A. Gomes , I. V. Gorelov , C. Gotti , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , E. Graverini , G. Graziani , A. Grecu , P. Griffith , L. Grillo , B. R. Gruberg Cazon , O. Grünberg , E. Gushchin , Yu. Guz , T. Gys , C. Göbel , T. Hadavizadeh , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , X. Han , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , J. He , T. Head , A. Heister , K. Hennessy , P. Henrard , L. Henry , J. A. Hernando Morata , E. van Herwijnen , M. Heß , A. Hicheur , D. Hill , C. Hombach , W. Hulsbergen , T. Humair , M. Hushchyn , N. Hussain , D. Hutchcroft , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , A. Jawahery , M. John , D. Johnson , C. R. Jones , C. Joram , B. Jost , N. Jurik , S. Kandybei , W. Kanso , M. Karacson , J. M. Kariuki , S. Karodia , M. Kecke , M. Kelsey , I. R. Kenyon , M. Kenzie , T. Ketel , E. Khairullin , B. Khanji , C. Khurewathanakul , T. Kirn , S. Klaver , K. Klimaszewski , S. Koliiev , M. Kolpin , I. Komarov , R. F. Koopman , P. Koppenburg , A. Kozachuk , M. Kozeiha , L. Kravchuk , K. Kreplin , M. Kreps , P. Krokovny , F. Kruse , W. Krzemien , W. Kucewicz , M. Kucharczyk , V. Kudryavtsev , A. K. Kuonen , K. Kurek , T. Kvaratskheliya , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , G. Lanfranchi , C. Langenbruch , B. Langhans , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , A. Leflat , J. Lefrançois , R. Lefèvre , F. Lemaitre , E. Lemos Cid , O. Leroy , T. Lesiak , B. Leverington , Y. Li , T. Likhomanenko , R. Lindner , C. Linn , F. Lionetto , B. Liu , X. Liu , D. Loh , I. Longstaff , J. H. Lopes , D. Lucchesi , M. Lucio Martinez , H. Luo , A. Lupato , E. Luppi , O. Lupton , A. Lusiani , X. Lyu , F. Machefert , F. Maciuc , O. Maev , K. Maguire , S. Malde , A. Malinin , T. Maltsev , G. Manca , G. Mancinelli , P. Manning , J. Maratas , J. F. Marchand , U. Marconi , C. Marin Benito , P. Marino , J. Marks , G. Martellotti , M. Martin , M. Martinelli , D. Martinez Santos , F. Martinez Vidal , D. Martins Tostes , L. M. Massacrier , A. Massafferri , R. Matev , A. Mathad , Z. Mathe , C. Matteuzzi , A. Mauri , B. Maurin , A. Mazurov , M. McCann , J. McCarthy , A. McNab , R. McNulty , B. Meadows , F. Meier , M. Meissner , D. Melnychuk , M. Merk , E Michielin , D. A. Milanes , M. -N. Minard , D. S. Mitzel , J. Molina Rodriguez , I. A. Monroy , S. Monteil , M. Morandin , P. Morawski , A. Mordà , M. J. Morello , J. Moron , A. B. Morris , R. Mountain , F. Muheim , M. Mulder , M. Mussini , D. Müller , J. Müller , K. Müller , V. Müller , P. Naik , T. Nakada , R. Nandakumar , A. Nandi , I. Nasteva , M. Needham , N. Neri , S. Neubert , N. Neufeld , M. Neuner , A. D. Nguyen , C. Nguyen-Mau , V. Niess , S. Nieswand , R. Niet , N. Nikitin , T. Nikodem , A. Novoselov , D. P. O'Hanlon , A. Oblakowska-Mucha , V. Obraztsov , S. Ogilvy , R. Oldeman , C. J. G. Onderwater , J. M. Otalora Goicochea , A. Otto , P. Owen , A. Oyanguren , A. Palano , F. Palombo , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , L. L. Pappalardo , C. Pappenheimer , W. Parker , C. Parkes , G. Passaleva , G. D. Patel , M. Patel , C. Patrignani , A. Pearce , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , P. Perret , L. Pescatore , K. Petridis , A. Petrolini , A. Petrov , M. Petruzzo , E. Picatoste Olloqui , B. Pietrzyk , M. Pikies , D. Pinci , A. Pistone , A. Piucci , S. Playfer , M. Plo Casasus , T. Poikela , F. Polci , A. Poluektov , I. Polyakov , E. Polycarpo , G. J. Pomery , A. Popov , D. Popov , B. Popovici , C. Potterat , E. Price , J. D. Price , J. Prisciandaro , A. Pritchard , C. Prouve , V. Pugatch , A. Puig Navarro , G. Punzi , W. Qian , R. Quagliani , B. Rachwal , J. H. Rademacker , M. Rama , M. Ramos Pernas , M. S. Rangel , I. Raniuk , G. Raven , F. Redi , S. Reichert , A. C. dos Reis , C. Remon Alepuz , V. Renaudin , S. Ricciardi , S. Richards , M. Rihl , K. Rinnert , V. Rives Molina , P. Robbe , A. B. Rodrigues , E. Rodrigues , J. A. Rodriguez Lopez , P. Rodriguez Perez , A. Rogozhnikov , S. Roiser , V. Romanovskiy , A. Romero Vidal , J. W. Ronayne , M. Rotondo , T. Ruf , P. Ruiz Valls , J. J. Saborido Silva , N. Sagidova , B. Saitta , V. Salustino Guimaraes , C. Sanchez Mayordomo , B. Sanmartin Sedes , R. Santacesaria , C. Santamarina Rios , M. Santimaria , E. Santovetti , A. Sarti , C. Satriano , A. Satta , D. M. Saunders , D. Savrina , S. Schael , M. Schiller , H. Schindler , M. Schlupp , M. Schmelling , T. Schmelzer , B. Schmidt , O. Schneider , A. Schopper , M. Schubiger , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , A. Semennikov , A. Sergi , N. Serra , J. Serrano , L. Sestini , P. Seyfert , M. Shapkin , I. Shapoval , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , B. G. Siddi , R. Silva Coutinho , L. Silva de Oliveira , G. Simi , M. Sirendi , N. Skidmore , T. Skwarnicki , E. Smith , I. T. Smith , J. Smith , M. Smith , H. Snoek , M. D. Sokoloff , F. J. P. Soler , D. Souza , B. Souza De Paula , B. Spaan , P. Spradlin , S. Sridharan , F. Stagni , M. Stahl , S. Stahl , P. Stefko , S. Stefkova , O. Steinkamp , O. Stenyakin , S. Stevenson , S. Stoica , S. Stone , B. Storaci , S. Stracka , M. Straticiuc , U. Straumann , L. Sun , W. Sutcliffe , K. Swientek , V. Syropoulos , M. Szczekowski , T. Szumlak , S. T'Jampens , A. Tayduganov , T. Tekampe , G. Tellarini , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Tolk , L. Tomassetti , D. Tonelli , S. Topp-Joergensen , E. Tournefier , S. Tourneur , K. Trabelsi , M. Traill , M. T. Tran , M. Tresch , A. Trisovic , A. Tsaregorodtsev , P. Tsopelas , A. Tully , N. Tuning , A. Ukleja , A. Ustyuzhanin , U. Uwer , C. Vacca , V. Vagnoni , S. Valat , G. Valenti , A. Vallier , R. Vazquez Gomez , P. Vazquez Regueiro , S. Vecchi , M. van Veghel , J. J. Velthuis , M. Veltri , G. Veneziano , A. Venkateswaran , M. Vesterinen , B. Viaud , D. Vieira , M. Vieites Diaz , X. Vilasis-Cardona , V. Volkov , A. Vollhardt , B. Voneki , D. Voong , A. Vorobyev , V. Vorobyev , C. Voß , J. A. de Vries , C. Vázquez Sierra , R. Waldi , C. Wallace , R. Wallace , J. Walsh , J. Wang , D. R. Ward , H. M. Wark , N. K. Watson , D. Websdale , A. Weiden , M. Whitehead , J. Wicht , G. Wilkinson , M. Wilkinson , M. Williams , M. P. Williams , M. Williams , T. Williams , F. F. Wilson , J. Wimberley , J. Wishahi , W. Wislicki , M. Witek , G. Wormser , S. A. Wotton , K. Wraight , S. Wright , K. Wyllie , Y. Xie , Z. Xing , Z. Xu , Z. Yang , H. Yin , J. Yu , X. Yuan , O. Yushchenko , M. Zangoli , K. A. Zarebski , M. Zavertyaev , L. Zhang , Y. Zhang , Y. Zhang , A. Zhelezov , Y. Zheng , A. Zhokhov , V. Zhukov , S. Zucchelli

A Higgs boson mass $\sim 126$ GeV as determined by the LHC data requires a large loop correction which in turn implies a large sfermion mass. Implication of this result for the stability of the proton in supersymmetric grand unified…

High Energy Physics - Phenomenology · Physics 2015-06-15 Mengxi Liu , Pran Nath

In principle, the baryon asymmetry of the Universe can be generated at the electroweak phase transition but the experimental lower limit on the Higgs mass seems to rule out a Standard Model scenario. However, it has been shown recently that…

High Energy Physics - Phenomenology · Physics 2009-02-16 D. Delepine

Observing a heavy charged Higgs boson produced in the near future at the Tevatron or at the LHC would be instant evidence of physics beyond the Standard Model. Whether such a Higgs boson would be supersymmetric or not it could only be…

High Energy Physics - Phenomenology · Physics 2010-01-28 J. A. Coarasa , David Garcia , Jaume Guasch , Ricardo A. Jimenez , Joan Sola

We discuss the lower Higgs boson mass bounds which come from the absolute stability of the Standard Model (SM) vacuum and from the Higgs inflation, as well as the prediction of the Higgs boson mass coming from asymptotic safety of the SM.…

High Energy Physics - Phenomenology · Physics 2015-06-05 Fedor Bezrukov , Mikhail Yu. Kalmykov , Bernd A. Kniehl , Mikhail Shaposhnikov

While the existence of a Higgs boson with a mass near 125 GeV has been clearly established, the detailed structure of the entire Higgs sector is yet unclear. Besides the Standard Model interpretation, various possibilities for extended…

High Energy Physics - Experiment · Physics 2015-06-19 Rainer Mankel

A toy model giving rise to long lived super heavy particles and an small vacuum density energy, of the order of the one measured in the present universe, is constructed. This model consists in hidden sector invariant under an $SU(2)_L$…

High Energy Physics - Theory · Physics 2012-08-29 O. P. Santillan

We evaluate the baryon number abundance based on the charge transport scenario of top quarks in the CP-violating two Higgs doublet model, in which Yukawa interactions are aligned to avoid dangerous flavor changing neutral currents, and…

High Energy Physics - Phenomenology · Physics 2022-01-25 Kazuki Enomoto , Shinya Kanemura , Yushi Mura
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