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Related papers: CKM studies from b physics at hadron machines

200 papers

LHCb is the dedicated B physics experiment at the LHC and is due to start data taking later this year. Its goal is to search for new physics in very rare processes and make precision measurements of CP violation in B decays. The CKM angle…

High Energy Physics - Experiment · Physics 2009-06-01 Ying Ying Li

Recent measurements have revealed a number of intriguing deviations from the Standard Model predictions in $B$ meson decays, in particular in observables testing lepton flavour universality. We review their experimental status and…

High Energy Physics - Phenomenology · Physics 2017-07-13 Monika Blanke

We currently live in the age of the CKM paradigm. The $3\times 3$ matrix that links $(d,\ s,\ b)$ quarks to $(u,\ c,\ t)$ in the charged current weak interaction, being complex and nominally with 18 parameters, can be accounted for by just…

High Energy Physics - Phenomenology · Physics 2017-10-25 Paoti Chang , Kai-Feng Chen , Wei-Shu Hou

We give a status report on quark flavour physics in view of the latest data from the B factories and the LHC, and discuss the impact of the latest experimental results on new physics in the MFV framework. We also show some examples of the…

High Energy Physics - Phenomenology · Physics 2013-05-21 Tobias Hurth , Farvah Mahmoudi

The physics underlying quark and lepton masses and mixings (the "flavor problem") is the least well understood aspect of the Standard Model. Some questions of flavor physics, and ways in which the LHC can help shed light on this problem,…

High Energy Physics - Phenomenology · Physics 2014-11-20 Jonathan L. Rosner

Thanks to the large cross-section for the production of strange and charm mesons at the Large Hadron Collider, LHCb has recently performed several new explorations of rare transitions that are highly suppressed or forbidden by the Standard…

High Energy Physics - Experiment · Physics 2024-04-01 Paras Naik

I review the current status of our knowledge of CP violation and flavor physics. I discuss where one should look for future improvements, and outline the experimental and theoretical priorities of the field.

High Energy Physics - Phenomenology · Physics 2014-11-17 Adam F. Falk

The role of charm in testing the Standard Model description of quark mixing and CP violation through measurements of lifetimes, decay constants and semileptonic form factors is reviewed. Together with Lattice QCD, charm has the potential…

High Energy Physics - Experiment · Physics 2008-11-26 I. Shipsey

In these three lectures, I overview the theoretical framework of the flavour physics and CP violation. The first lecture is the introduction to the flavour physics. Namely, I give theoretical basics of the weak interaction. I follow also…

High Energy Physics - Phenomenology · Physics 2014-07-01 Emi Kou

Although direct detection of new particles will be the main focus of the LHC, indirect New Physics searches are expected to provide useful complementary information. In particular, precision measurements of rare processes occurring in…

High Energy Physics - Experiment · Physics 2008-05-19 A. Hicheur

We review flavour and CP violations in the lepton sector as probes of new physics beyond the standard model and its minimal extensions accommodating massive neutrinos. After recalling the main experimental bounds and the future…

High Energy Physics - Phenomenology · Physics 2015-09-29 Ferruccio Feruglio

Lectures on flavor physics presented at the 2012 CERN HEP Summer School. Content: 1) flavor physics within the Standard Model, 2) phenomenology of B and D decays, 3) flavor physics beyond the Standard Model.

High Energy Physics - Phenomenology · Physics 2013-02-05 Gino Isidori

Run 2 of the LHC offers some beautiful prospects for new physics, including flavour physics as well as more detailed studies of the Higgs boson and searches for new physics beyond the Standard Model (BSM). One of the possibilities for BSM…

High Energy Physics - Phenomenology · Physics 2014-12-09 John Ellis

With the advent of the LHC, we will be able to probe New Physics (NP) up to energy scales almost one order of magnitude larger than it has been possible with present accelerator facilities. While direct detection of new particles will be…

High Energy Physics - Phenomenology · Physics 2010-05-27 G. Buchalla , T. K. Komatsubara , F. Muheim , L. Silvestrini , M. Artuso , D. M. Asner , P. Ball , E. Baracchini , G. Bell , M. Beneke , J. Berryhill , A. Bevan , I. I. Bigi , M. Blanke , Ch. Bobeth , M. Bona , F. Borzumati , T. Browder , T. Buanes , O. Buchmuller , A. J. Buras , S. Burdin , D. G. Cassel , R. Cavanaugh , M. Ciuchini , P. Colangelo , G. Crosetti , A. Dedes , F. De Fazio , S. Descotes-Genon , J. Dickens , Z. Dolezal , S. Durr , U. Egede , C. Eggel , G. Eigen , S. Fajfer , Th. Feldmann , R. Ferrandes , P. Gambino , T. Gershon , V. Gibson , M. Giorgi , V. V. Gligorov , B. Golob , A. Golutvin , Y. Grossman , D. Guadagnoli , U. Haisch , M. Hazumi , S. Heinemeyer , G. Hiller , D. Hitlin , T. Huber , T. Hurth , T. Iijima , A. Ishikawa , G. Isidori , S. Jager , A. Khodjamirian , P. Koppenburg , T. Lagouri , U. Langenegger , C. Lazzeroni , A. Lenz , V. Lubicz , W. Lucha , H. Mahlke , D. Melikhov , F. Mescia , M. Misiak , M. Nakao , J. Napolitano , N. Nikitin , U. Nierste , K. Oide , Y. Okada , P. Paradisi , F. Parodi , M. Patel , A. A. Petrov , T. N. Pham , M. Pierini , S. Playfer , G. Polesello , A. Policicchio , A. Poschenrieder , P. Raimondi , S. Recksiegel , P. Reznicek , A. Robert , S. Robertson , J. L. Rosner , G. Ruggiero , A. Sarti , O. Schneider , F. Schwab , S. Simula , S. Sivoklokov , P. Slavich , C. Smith , M. Smizanska , A. Soni , T. Speer , P. Spradlin , M. Spranger , A. Starodumov , B. Stech , A. Stocchi , S. Stone , C. Tarantino , F. Teubert , S. T'Jampens , K. Toms , K. Trabelsi , S. Trine , S. Uhlig , V. Vagnoni , J. J. van Hunen , G. Weiglein , A. Weiler , G. Wilkinson , Y. Xie , M. Yamauchi , G. Zhu , J. Zupan , R. Zwicky

We present the results of an extensive analysis of flavour physics in both quark and lepton sectors, in the Littlest Higgs model with T-parity (LHT). In the quark sector, we identify some interesting scenarios for new mirror quark masses…

High Energy Physics - Phenomenology · Physics 2011-03-23 Cecilia Tarantino

The Littlest Higgs Model with T-parity (LHT) belongs to the simplest new physics scenarios with new sources of flavour and CP violation. We present a new analysis of quark observables in the LHT model in view of the oncoming flavour…

High Energy Physics - Phenomenology · Physics 2016-04-07 Monika Blanke , Andrzej J. Buras , Stefan Recksiegel

The LHC physics era is about to commence; here we discuss a complementary physics program that would be realized at a high luminosity flavor factory. A flavor factory experiment can search for new physics in CP asymmetries, inclusive decay…

High Energy Physics - Experiment · Physics 2009-09-25 A. J. Schwartz

Measurements of $CP$-violating observables in $B$ meson decays can be used to determine the angles of the Unitarity Triangle and hence probe for manifestations of New Physics beyond the Cabibbo-Kobayashi-Maskawa Standard Model paradigm. Of…

High Energy Physics - Experiment · Physics 2017-08-30 Greig A. Cowan

We present an overview of what we learned so far from low-energy flavour observables, concerning physics beyond the Standard Model, and what we could still learn from further studies in flavour physics in the next few years.

High Energy Physics - Phenomenology · Physics 2008-01-22 Gino Isidori

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