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Related papers: Flavour and Higgs compositeness: present and "near…

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We study the lepton sector of composite Higgs models with partial compositeness. The standard anarchic scenario is in conflict with the absence of observable charged lepton flavor violation. This tension can be completely solved in MFV…

High Energy Physics - Phenomenology · Physics 2015-06-16 Michele Redi

Composite Higgs models are an attractive scenario, where the discovered Higgs boson is regarded as a Nambu-Goldstone boson associated with spontaneous breakdown of a global symmetry of more fundamental theory. This class of models predicts…

High Energy Physics - Phenomenology · Physics 2015-04-30 Kunio Kaneta

We continue our investigation of gauge theories in which the Higgs boson arises as a pseudo-Nambu-Goldstone boson (pNGB) and top-partners arise as bound states of three hyperfermions. All models have additional pNGBs in their spectrum that…

High Energy Physics - Phenomenology · Physics 2016-07-20 Gabriele Ferretti

With no evidence of any exotic particle detected so far beyond the Standard Model, the new physics may lie above the presently accessible energies at colliders and, at low-energies, can be accounted for via an effective description. The…

High Energy Physics - Phenomenology · Physics 2023-08-21 Arturo de Giorgi , Fotis Koutroulis , Luca Merlo , Stefan Pokorski

We present a simple microscopic realization of a pseudo-Nambu-Goldstone (pNGB) boson Higgs scenario arising from the breaking of $SO(5) \rightarrow SO(4)$. The Higgs constituents are explicitly identified as well as the interactions…

High Energy Physics - Phenomenology · Physics 2015-07-20 Gero von Gersdorff , Eduardo Ponton , Rogerio Rosenfeld

This Thesis is devoted to the phenomenological analysis at the large hadron collider (LHC), as well at a future electron positron collider, of the 4 dimensional (4D) composite Higgs model (4DCHM), a compelling beyond the standard model…

High Energy Physics - Phenomenology · Physics 2014-11-24 Daniele Barducci

In these proceedings we review the impact of additional Higgs bosons on $B$ physics observables. For this purpose, we consider first the 2HDM of type II which respects natural flavour conservation. Afterwards, we study a 2HDM with generic…

High Energy Physics - Phenomenology · Physics 2014-12-09 Andreas Crivellin

We present a framework to study the interactions among Nambu-Goldstone bosons (NGB), pseudo-NGB (pNGBs) and gauge bosons in Composite Higgs (CH) models at high energies, including operators of order $\mathcal{O}(p^4)$ and…

High Energy Physics - Phenomenology · Physics 2023-02-07 Diogo Buarque Franzosi

We present a unified picture of flavor and electroweak symmetry breaking based on a nonlinear sigma model spontaneously broken at the TeV scale. Flavor and Higgs bosons arise as pseudo-Goldstone modes. Explicit collective symmetry breaking…

High Energy Physics - Phenomenology · Physics 2009-11-10 Federica Bazzocchi , Marco Fabbrichesi

We describe recent work on the physics of the Higgs boson at future muon colliders. Starting from the low energy muon collider at the Higgs boson pole we extend our discussion to the multi-TeV muon collider and outline the physics case for…

High Energy Physics - Phenomenology · Physics 2021-04-14 Roberto Franceschini , Mario Greco

The Littlest Higgs Model with T parity (LHT) is an interesting alternative model for New Physics at the TeV scale. Although Flavour Physics was not the reason for creating the LHT model, significant effects (such as large CP violation where…

High Energy Physics - Phenomenology · Physics 2015-05-14 Stefan Recksiegel

Motivated by the success of the flavour physics programme carried out over the last decade at the Large Hadron Collider (LHC), we characterize in detail the physics potential of its High-Luminosity and High-Energy upgrades in this domain of…

High Energy Physics - Phenomenology · Physics 2019-02-25 A. Cerri , V. V. Gligorov , S. Malvezzi , J. Martin Camalich , J. Zupan , S. Akar , J. Alimena , B. C. Allanach , W. Altmannshofer , L. Anderlini , F. Archilli , P. Azzi , S. Banerjee , W. Barter , A. E. Barton , M. Bauer , I. Belyaev , S. Benson , M. Bettler , R. Bhattacharya , S. Bifani , A. Birnkraut , F. Bishara , T. Blake , S. Blusk , E. Boos , M. Borsato , C. Bozzi , A. Bragagnolo , J. Brod , J. Brodzicka , A. J. Buras , L. Cadamuro , A. Carbone , M. Carena , I. Carli , A. Carmona , F. R. Cavallo , A. Celis , M. Cepeda , G. S. Chahal , M. Chala , J. Charles , M. Charles , K. F. Chen , V. Chobanova , M. Chrzaszcz , G. Ciezarek , V. Cirigliano , M. Ciuchini , H. Cliff , J. Cogan , G. Colangelo , A. Contu , R. Covarelli , G. Cowan , A. Crivellin , G. D'Ambrosio , M. D'Onofrio , N. P. Dang , A. Davis , O. A. De Aguiar Francisco , K. De Bruyn , U. De Sanctis , H. De la Torre , W. Dekens , F. Deliot , M. Della Morte , S. Demers , D. Derkach , O. Deschamps , S. Descotes-Genon , F. Dettori , A. Di Canto , M. Dinardo , P. Dini , F. Dordei , M. Dorigo , A. dos Reis , L. Dudko , L. Dufour , G. Durieux , S. Dutta , A. Dziurda , U. Eitschberger , A. Esposito , M. Estevez , S. Fajfer , A. Falkowski , D. A. Faroughy , G. Fedi , S. Fiorendi , F. Fiori , C. Fitzpatrick , R. Fleischer , M. Fontana , P. J. Fox , M. Freytsis , E. Gámiz , E. Gabriel , P. Gambino , J. García Pardiñas , L. S. Geng , E. Gersabeck , M. Gersabeck , T. Gershon , A. Gilbert , M. Gonzalez-Alonso , P. Govoni , G. Graziani , A. Greljo , L. Grillo , B. Grinstein , A. Grohsjean , Y. Grossman , D. Guadagnoli , F. -K. Guo , L. Guzzi , J. Haller , B. Hamilton , T. Han , R. Harnik , D. Hill , G. Hiller , K. Hoepfner , J. M. Hogan , T. Hurth , O. Igonkina , P. Ilten , G. Isidori , Sa. Jain , M. John , D. Johnson , M. Jung , N. Jurik , S. Jäger , M. Kado , A. L. Kagan , J. F. Kamenik , M. Karliner , M. Kenzie , B. Khanji , J. Kieseler , T. Kitahara , T. Klijnsma , M. Knecht , N. Košnik , R. Kogler , P. Koppenburg , A. Korytov , M. Kreps , C. Langenbruch , U. Langenegger , T. Latham , R. F. Lebed , A. J. Lenz , N. Leonardo , O. Leroy , Q. Li , T. Li , F. Ligabue , Z. Ligeti , K. Long , E. Lunghi , F. Mahmoudi , G. Mancinelli , P. Mandrik , T. Mannel , X. Marcano , J. F. Marchand , D. Martínez Santos , A. Martin , M. Martinelli , F. Martinez Vidal , D. Marzocca , J. Matias , P. Matorras Cuevas , O. Matsedonskyi , A. Mauri , K. Mazumdar , M. Merk , A. B. Meyer , E. Michielin , G. Mitselmakher , L. Mittnacht , S. Monteil , M. J. Morello , M. Morgenstern , M. Narain , M. Nardecchia , M. Needham , N. Neri , M. Neubert , S. Neubert , U. Nierste , J. Nieves , Y. Nir , A. Nisati , D. P. O'Hanlon , E. Oset , P. Owen , O. Ozcelik , S. Pagan Griso , E. Palencia Cortezon , F. Palla , M. Palutan , M. Pappagallo , C. Parkes , S. Pascoli , G. Passaleva , E. Passemar , M. Patel , A. Pearce , K. Pedro , S. Perazzini , M. Perfilov , L. Perrozzi , L. Pescatore , B. A. Petersen , A. A. Petrov , A. Pich , A. Pilloni , F. Polci , A. D. Polosa , S. Prelovsek , A. Puig Navarro , G. Punzi , J. Rademacker , M. Rama , M. Reboud , A. Reimers , P. Reznicek , D. J. Robinson , J. L. Rosner , R. Ruiz , S. Saito , S. Sarkar , A. Savin , S. Sawant , S. Schacht , M. Schlaffer , A. Schmidt , B. Schneider , A. Schopper , M. H. Schune , J. Segovia , M. Selvaggi , N. Serra , G. Servant , L. Sestini , D. Shih , R. Silva Coutinho , L. Silvestrini , K. Skovpen , T. Skwarnicki , M. Smizanska , A. Soni , Y. Soreq , M. Spannowsky , P. Spradlin , E. Stamou , S. Stone , S. Stracka , D. M. Straub , A. P Szczepaniak , S. T'Jampens , Y. Takahashi , F. Teubert , E. Thomas , V. Tisserand , R. Torre , F. Tresoldi , D. Tsiakkouri , S. Turchikhin , K. A. Ulmer , V. Vagnoni , D. van Dyk , J. van Tilburg , S. Vecchi , R. Venditti , M. Vesterinen , J. Virto , P. Volkov , G. Vorotnikov , E. Vryonidou , J. Walder , W. Walkowiak , J. Wang , W. Wang , C. Weiland , M. Whitehead , G. Wilkinson , J. M. Williams , M. R. J. Williams , F. Wilson , Y. Xie , Z. Yang , E. Yazgan , T. You , F. Yu , C. Zhang , L. Zhang , W. Zhang

We investigate the possibility that Dark Matter arises as a composite state of a fundamental confining dynamics, together with the Higgs boson. We focus on the minimal SU(4)$\times$SU(4)/SU(4) model which has both a Dark Matter and a Higgs…

High Energy Physics - Phenomenology · Physics 2017-08-22 Teng Ma , Yongcheng Wu , Bin Zhang , Giacomo Cacciapaglia

The rather precise knowledge of the mass of the Higgs boson and of its couplings has important consequences for the physical phenomena taking place at the Fermi scale. We analyze some of these implications in the most motivated frameworks…

High Energy Physics - Phenomenology · Physics 2014-03-27 Dario Buttazzo

Composite Higgs models are an intriguing scenario in which the Higgs particle is identified as a pseudo Nambu-Goldstone boson associated with spontaneous breaking of some global symmetry above the electroweak scale. They would predict new…

High Energy Physics - Phenomenology · Physics 2015-03-17 Shinya Kanemura , Kunio Kaneta , Naoki Machida , Tetsuo Shindou

Composite Higgs models can trivially satisfy precision-electroweak and flavour constraints by simply having a large spontaneous symmetry breaking scale, f > 10 TeV. This produces a 'split' spectrum, where the strong sector resonances have…

High Energy Physics - Phenomenology · Physics 2015-06-23 James Barnard , Tony Gherghetta , Tirtha Sankar Ray , Andrew Spray

We give a brief introduction to flavour physics. The first part covers the flavour structure of the Standard Model, how the Kobayashi-Maskawa mechanism is tested and provides examples of searches for new physics using flavour observables,…

High Energy Physics - Phenomenology · Physics 2019-04-04 Jure Zupan

We present a unified picture of flavor and electroweak symmetry breaking at the TeV scale. Flavor and Higgs bosons arise as pseudo-Goldstone modes in a nonlinear sigma model. Explicit collective symmetry breaking yields stable vacuum…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Bazzocchi , M. Fabbrichesi

We consider the flavour problem in a supersymmetric Grand Unified theory with gauged SU(6) group, where the Higgs doublets are understood as pseudo-Goldstone bosons of a larger $\SU(6)\otimes\SU(6)$ global symmetry of the Higgs…

High Energy Physics - Phenomenology · Physics 2009-10-09 R. Barbieri , Z. Berezhiani , G. Dvali , L. Hall , A. Strumia

The future of flavour physics and CP violation in the quark, lepton and Higgs sectors are discussed, particularly from the viewpoint of physics beyond the Standard Model, such as supersymmetry. Current issues in B to pi^+ pi^-, phi K_s and…

High Energy Physics - Phenomenology · Physics 2009-09-11 John Ellis