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Related papers: Composite Higgs under LHC Experimental Scrutiny

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Composite particles generated by an unknown strong dynamics can be responsible for the ElectroWeak Symmetry Breaking (EWSB) and can substitute the Standard Model (SM) Higgs boson in keeping perturbative unitarity in the longitudinal WW…

High Energy Physics - Phenomenology · Physics 2011-10-19 Riccardo Torre

In a composite model of the weak bosons the p-wave bosons are studied. The state with the lowest mass is identified with the boson, which might have been detected recently at the LHC. Specific properties of these excited bosons are studied,…

High Energy Physics - Phenomenology · Physics 2015-06-04 Harald Fritzsch

In the post-Higgs discovery era, the primary goal of the Large Hadron collider is to discover new physics Beyond the Standard Model. One fundamental question is does new beyond the Standard Model composite dynamics provides the origin of…

High Energy Physics - Lattice · Physics 2020-05-05 V. Drach

In scenarios of strongly coupled electroweak symmetry breaking, heavy composite particles of different spin and parity may arise and cause observable effects on signals that appear at loop levels. The recently observed process of Higgs to…

High Energy Physics - Phenomenology · Physics 2015-10-27 A. E. Cárcamo Hernández , Claudio O. Dib , Alfonso R. Zerwekh

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

The recently announced Higgs discovery marks the dawn of the direct probing of the electroweak symmetry breaking sector. Sorting out the dynamics responsible for electroweak symmetry breaking now requires probing the Higgs interactions and…

High Energy Physics - Phenomenology · Physics 2014-02-12 Tyler Corbett , O. J. P. Eboli , J. Gonzalez-Fraile , M. C. Gonzalez-Garcia

We propose a four dimensional description of Composite Higgs Models which represents a complete framework for the physics of the Higgs as a pseudo-Nambu-Goldstone boson. Our setup captures all the relevant features of 5D models and more in…

High Energy Physics - Phenomenology · Physics 2014-03-03 Stefania De Curtis , Michele Redi , Andrea Tesi

We present an overview of composite Higgs models in light of the discovery of the Higgs boson. The small value of the physical Higgs mass suggests that the Higgs quartic is likely loop generated, thus models with tree-level quartics will…

High Energy Physics - Phenomenology · Physics 2015-06-18 Brando Bellazzini , Csaba Csáki , Javi Serra

Now that a Higgs boson has been discovered at the LHC, measuring its couplings to other particles is the next important step. In order to probe the electroweak symmetry breaking mechanism at its core it is crucial to reconstruct the scalar…

High Energy Physics - Phenomenology · Physics 2014-08-28 Julien Baglio

If electroweak symmetry breaking arises via strong dynamics, electroweak precision tests and flavour physics experiments suggest that the minimal model should closely resemble the Standard Model at the LHC. I describe two directions going…

High Energy Physics - Phenomenology · Physics 2010-05-07 Ben Gripaios

An essential goal of the Higgs physics program at the LHC and beyond is to explore the nature of the Higgs potential and shed light on the mechanism of electroweak symmetry breaking. An important class of models defining the strength and…

High Energy Physics - Phenomenology · Physics 2022-03-17 Marcela Carena , Jonathan Kozaczuk , Zhen Liu , Tong Ou , Michael J. Ramsey-Musolf , Jessie Shelton , Yikun Wang , Ke-Pan Xie

The cause of the screening of the weak interactions at long distances puzzled the high-energy community for more nearly half a century. With the discovery of the Higgs boson a new era started with direct experimental information on the…

High Energy Physics - Phenomenology · Physics 2017-08-03 C. Grojean

The discovery of the Higgs boson in 2012, by the ATLAS and CMS experiments, was a success achieved with only a percent of the entire dataset foreseen for the LHC. It opened a landscape of possibilities in the study of Higgs boson…

High Energy Physics - Phenomenology · Physics 2019-03-20 M. Cepeda , S. Gori , P. Ilten , M. Kado , F. Riva , R. Abdul Khalek , A. Aboubrahim , J. Alimena , S. Alioli , A. Alves , C. Asawatangtrakuldee , A. Azatov , P. Azzi , S. Bailey , S. Banerjee , E. L. Barberio , D. Barducci , G. Barone , M. Bauer , C. Bautista , P. Bechtle , K. Becker , A. Benaglia , M. Bengala , N. Berger , C. Bertella , A. Bethani , A. Betti , A. Biekotter , F. Bishara , D. Bloch , P. Bokan , O. Bondu , M. Bonvini , L. Borgonovi , M. Borsato , S. Boselli , S. Braibant-Giacomelli , G. Buchalla , L. Cadamuro , C. Caillol , A. Calandri , A. Calderon Tazon , J. M. Campbell , F. Caola , M. Capozi , M. Carena , C. M. Carloni Calame , A. Carmona , E. Carquin , A. Carvalho Antunes De Oliveira , A. Castaneda Hernandez , O. Cata , A. Celis , A. Cerri , F. Cerutti , G. S. Chahal , A. Chakraborty , G. Chaudhary , X. Chen , A. S. Chisholm , R. Contino , A. J. Costa , R. Covarelli , N. Craig , D. Curtin , L. D'Eramo , N. P. Dang , P. Das , S. Dawson , O. A. De Aguiar Francisco , J. de Blas , S. De Curtis , N. De Filippis , H. De la Torre , L. de Lima , A. De Wit , C. Delaere , M. Delcourt , M. Delmastro , S. Demers , N. Dev , R. Di Nardo , S. Di Vita , S. Dildick , L. A. F. do Prado , M. Donadelli , D. Du , G. Durieux , M. Dührssen , O. Eberhardt , K. El Morabit , J. Elias-Miro , J. Ellis , C. Englert , R. Essig , S. Falke , M. Farina , A. Ferrari , A. Ferroglia , M. C. N. Fiolhais , M. Flechl , S. Folgueras , E. Fontanesi , P. Francavilla , R. Franceschini , R. Frederix , S. Frixione , G. Gómez-Ceballos , A. Gabrielli , S. Gadatsch , M. Gallinaro , A. Gandrakota , J. Gao , F. M. Garay Walls , T. Gehrmann , Y. Gershtein , T. Ghosh , A. Gilbert , R. Glein , E. W. N. Glover , R. Gomez-Ambrosio , R. Gonçalo , D. Gonçalves , M. Gorbahn , E. Gouveia , M. Gouzevitch , P. Govoni , M. Grazzini , B. Greenberg , K. Grimm , A. V. Gritsan , A. Grohsjean , C. Grojean , J. Gu , R. Gugel , R. S. Gupta , C. B. Gwilliam , S. Höche , M. Haacke , Y. Haddad , U. Haisch , G. N. Hamity , T. Han , L. A. Harland-Lang , R. Harnik , S. Heinemeyer , G. Heinrich , B. Henning , V. Hirschi , K. Hoepfner , J. M. Hogan , S. Homiller , Y. Huang , A. Huss , S. Jézéquel , Sa. Jain , S. P. Jones , K. Köneke , J. Kalinowski , J. F. Kamenik , M. Kaplan , A. Karlberg , M. Kaur , P. Keicher , M. Kerner , A. Khanov , J. Kieseler , J. H. Kim , M. Kim , T. Klijnsma , F. Kling , M. Klute , J. R. Komaragiri , K. Kong , J. Kozaczuk , P Kozow , C. Krause , S. Lai , J. Langford , B. Le , L. Lechner , W. A. Leight , K. J. C. Leney , T. Lenz , C-Q. Li , H. Li , Q. Li , S. Liebler , J. Lindert , D. Liu , J. Liu , Y. Liu , Z. Liu , D. Lombardo , A. Long , K. Long , I. Low , G. Luisoni , L. L. Ma , A. -M. Magnan , D. Majumder , A. Malinauskas , F. Maltoni , M. L. Mangano , G. Marchiori , A. C. Marini , A. Martin , S. Marzani , A. Massironi , K. T. Matchev , R. D. Matheus , K. Mazumdar , J. Mazzitelli , A. E. Mcdougall , P. Meade , P. Meridiani , A. B. Meyer , E. Michielin , P. Milenovic , V. Milosevic , K. Mimasu , B. Mistlberger , M. Mlynarikova , M. Mondragon , P. F. Monni , G. Montagna , F. Monti , M. Moreno Llacer , A. Mueck , P. C. Muiño , C. Murphy , W. J. Murray , P. Musella , M. Narain , R. F. Naranjo Garcia , P. Nath , M. Neubert , O. Nicrosini , K. Nikolopoulos , A. Nisati , J. M. No , M. L. Ojeda , S. A. Olivares Pino , A. Onofre , G. Ortona , S. Pagan Griso , D. Pagani , E. Palencia Cortezon , C. Palmer , C. Pandini , G. Panico , L. Panwar , D. Pappadopulo , M. Park , R. Patel , F. Paucar-Velasquez , K. Pedro , L. Pernie , L. Perrozzi , B. A. Petersen , E. Petit , G. Petrucciani , G. Piacquadio , F. Piccinini , M. Pieri , T. Plehn , S. Pokorski , A. Pomarol , E. Ponton , S. Pozzorini , S. Prestel , K. Prokofiev , M. Ramsey-Musolf , E. Re , N. P. Readioff , D. Redigolo , L. Reina , E. Reynolds , M. Riembau , F. Rikkert , T. Robens , R. Roentsch , J. Rojo , N. Rompotis , J. Rorie , J. Rosiek , J. Roskes , J. T. Ruderman , N. Sahoo , S. Saito , R. Salerno , P. H. Sales De Bruin , A. Salvucci , K. Sandeep , J. Santiago , R. Santo , V. Sanz , U. Sarica , A. Savin , A. Savoy-Navarro , S. Sawant , A. C. Schaffer , M. Schlaffer , A. Schmidt , B. Schneider , R. Schoefbeck , M. Schröder , M. Scodeggio , E. Scott , L. Scyboz , M. Selvaggi , L. Sestini , H. -S. Shao , A. Shivaji , L. Silvestrini , L. Simon , K. Sinha , Y. Soreq , M. Spannowsky , M. Spira , D. Spitzbart , E. Stamou , J. Stark , T. Stefaniak , B. Stieger , G. Strong , M. Szleper , K. Tackmann , M. Takeuchi , S. Taroni , M. Testa , A. Thamm , V. Theeuwes , L. A. Thomsen , S. Tkaczyk , R. Torre , F. Tramontano , K. A. Ulmer , T. Vantalon , L. Vecchi , R. Vega-Morales , E. Venturini , M. Verducci , C. Vernieri , T. Vickey , M. Vidal Marono , P. Vischia , E. Vryonidou , P. Wagner , V. M. Walbrecht , L. -T. Wang , N. Wardle , D. R. Wardrope , G. Weiglein , S. Wertz , M. Wielers , J. M. Williams , R. Wolf , A. Wulzer , M. Xiao , H. T. Yang , E. Yazgan , Z. Yin , T. You , F. Yu , G. Zanderighi , D. Zanzi , M. Zaro , S. C. Zenz , D. Zerwas , M. Zgubič , J. Zhang , L. Zhang , W. Zhang , X. Zhao , Y. -M. Zhong

The strategies recently developed to study Higgs boson properties at the LHC are reviewed. It is shown how to obtain model-independent determinations of couplings to fermions and gauge bosons by exploiting different production and decay…

High Energy Physics - Phenomenology · Physics 2011-09-13 Mauro Moretti

The Higgs low-energy theorem gives a simple and elegant way to estimate the couplings of the Higgs boson to massless gluons and photons induced by loops of heavy particles. We extend this theorem to take into account possible nonlinear…

High Energy Physics - Phenomenology · Physics 2015-03-20 M. Gillioz , R. Grober , C. Grojean , M. Muhlleitner , E. Salvioni

Higgs boson compositeness is a phenomenologically viable scenario addressing the hierarchy problem. In minimal models, the Higgs boson is the only degree of freedom of the strong sector below the strong interaction scale. We present here…

High Energy Physics - Phenomenology · Physics 2017-09-27 Mikael Chala , Gauthier Durieux , Christophe Grojean , Leonardo de Lima , Oleksii Matsedonskyi

Pairs of standard model fermions can annihilate to produce mini black holes with gauge quantum numbers of the Higgs boson at $M_{Planck}$. This leads to a Nambu-Jona-Lasinio model at the Planck scale with strong coupling which binds fermion…

High Energy Physics - Phenomenology · Physics 2020-07-23 Christopher T. Hill

The LHC potential for observing a light Higgs boson produced through Weak Boson Fusion mode, ${\rm qq}\to {\rm qqH}$, is presented. For non-hadronic decays modes of the Higgs boson the process is identified with a final state containing two…

High Energy Physics - Experiment · Physics 2007-05-23 K. Mazumdar

The discovery of a light Higgs boson at the LHC opens a broad program of studies and measurements to understand the role of this particle in connection with New Physics and Cosmology. Supersymmetry is the best motivated and most thoroughly…

High Energy Physics - Phenomenology · Physics 2016-04-20 Alexandre Arbey , Marco Battaglia , Farvah Mahmoudi

We consider a scenario of a composite Higgs arising from a strong sector. We assume that the lowest lying composite states are the Higgs scalar doublet and a massive vector triplet, whose dynamics below the compositeness scale are described…

High Energy Physics - Phenomenology · Physics 2018-01-03 A. E. Cárcamo Hernández , Bastián Díaz Sáez , Claudio O. Dib , Alfonso Zerwekh