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Related papers: Inclusive Flavour Tagging Algorithm

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In the last years, the \lhcb experiment established itself as an important contributor to heavy ion physics by exploiting some of its specific features. Production of particles, notably heavy flavour states, can be studied in p-p, p-Pb and…

High Energy Physics - Experiment · Physics 2019-10-02 Giacomo Graziani

Searches for lepton flavor violation (LFV) stand at the forefront of experimental particle physics research, offering a sensitive probe to many scenarios of physics beyond the Standard Model. The high proton-proton collision energy and…

High Energy Physics - Experiment · Physics 2024-03-20 Jian Wang

The experimental success of the predictions of the Standard Model in the flavour sector suggests that New Physics should possess a highly non-generic flavour structure. Different approaches to this idea of Minimal Flavour Violation have…

High Energy Physics - Phenomenology · Physics 2014-08-19 Maria Valentina Carlucci

At the Large Hadron Collider, the identification of jets originating from b quarks is important for searches for new physics and for measurements of standard model processes. A variety of algorithms has been developed by CMS to select…

High Energy Physics - Experiment · Physics 2013-05-30 CMS Collaboration

A second major upgrade of the LHCb detector is necessary to allow full exploitation of the HL-LHC for flavour physics. The new detector will be installed during long shutdown 4 (LS4), and will operate at instantaneous luminosity up to $1.5…

High Energy Physics - Experiment · Physics 2025-04-01 LHCb collaboration

The conventional description of heavy-flavour hadron production in pp collisions is based on a factorisation approach, assuming universal fragmentation functions among collision systems. Recent results on heavy-flavour baryon measurements…

High Energy Physics - Experiment · Physics 2021-09-21 Mattia Faggin

The LHCb Experiment is preparing a detector upgrade fully exploit the flavour physics potential of the LHC. The whole detector will be read out at the full collision rate and the online event selection will be performed by a software…

Instrumentation and Detectors · Physics 2017-09-15 Lars Eklund

The ALICE experiment at the LHC was taking data in proton-proton collisions at the center-of-mass energy of 7 TeV starting from March till the end of October 2010. First heavy-ion collisions were delivered during November 2010. Among other…

High Energy Physics - Experiment · Physics 2013-04-09 Serhiy Senyukov for ALICE collaboration

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 consider the inclusive reaction \ell^+ \ell^- -> nb +X (n = number of b-jets) in lepton colliders for which we propose a useful approximately conserved quantum number b_P=(-1)^n that we call b-Parity (b_P). We make the observation that…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Bar-Shalom , J. Wudka

Thanks to the excellent tracking and muon identification performance, combined with a flexible trigger system, the CMS experiment at the Large Hadron Collider is conducting a rich and competitive program of measurements in the field of…

High Energy Physics - Experiment · Physics 2019-08-13 Vincenzo Chiochia

Heavy flavor production at the future Electron-Ion Collider (EIC) will allow us to precisely determine the quark/gluon fragmentation processes in vacuum and the nuclear medium especially within the poorly constrained kinematic region. Heavy…

Nuclear Experiment · Physics 2022-07-13 Xuan Li

Many measurements and searches for physics beyond the standard model at the LHC rely on the efficient identification of heavy-flavour jets, i.e. jets originating from bottom or charm quarks. In this paper, the discriminating variables and…

Instrumentation and Detectors · Physics 2018-05-10 CMS Collaboration

We employ an approximate conserved quantum number (defined as "$b$-Parity" in [1]) of the Standard Model (SM): $b_P=(-1)^n$, where $n$ is the number of produced $b$-jets in the reaction $e + p/A \to n \cdot j_b +X$, to explore new TeV-scale…

High Energy Physics - Phenomenology · Physics 2026-01-08 Shaouly Bar-Shalom , Jose Wudka

The proposed high-energy and high-luminosity Electron-Ion Collider (EIC) will provide one of the cleanest environments to precisely determine the nuclear parton distribution functions (nPDFs) in a wide $x$-$Q^{2}$ range. Heavy flavor…

We introduce the idea of flavour transfer from a non-abelian horizontal $SU(2)_f$ flavour gauge group embedded in the Standard Model flavour structure. The new flavour vector bosons, in the mass range from the tens of GeV to multi-TeV do…

High Energy Physics - Phenomenology · Physics 2024-06-21 Luc Darmé , Aldo Deandrea , Farvah Mahmoudi

In this talk, I will present the status of lepton flavor physics in composite Higgs models with partial compositeness in the light of recent data in the lepton sector. I will consider anarchic flavor setups, scenarios with flavor…

High Energy Physics - Phenomenology · Physics 2021-12-03 Florian Goertz

The identification of b jets is a crucial issue to study and characterize various channels like top quark events and many new physics scenarios. Different b-tagging techniques are defined in CMS which benefit from the long life time, high…

High Energy Physics - Experiment · Physics 2012-01-26 Cristina Ferro

The interplay of flavour and collider physics is entering a new era with the start-up of the LHC. During the past few years rare B decays and in particular b -> s gamma transitions have been extensively used and provided exciting…

High Energy Physics - Phenomenology · Physics 2010-12-01 F. Mahmoudi
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