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Chapter 12 in High-Luminosity Large Hadron Collider (HL-LHC) : Preliminary Design Report. The Large Hadron Collider (LHC) is one of the largest scientific instruments ever built. Since opening up a new energy frontier for exploration in…

Accelerator Physics · Physics 2017-05-31 V. Baglin , P. Chiggiato , P. Cruikshank , M. Gallilee , C. Garion , R. Kersevan

The LHCb experiment will search for New Physics in Bs mixing. The Bs mixing phase will be extracted from the measurement of the time-dependent CP asymmetry in exclusive Bs decays governed by the b -> ccbar s quark-level transition. Large…

High Energy Physics - Experiment · Physics 2007-10-30 LHCb collaboration , Johan Blouw

Real-time data processing is a central aspect of particle physics experiments with high requirements on computing resources. The LHCb experiment must cope with the 30 million proton-proton bunches collision per second rate of the Large…

Chapter 6 in High-Luminosity Large Hadron Collider (HL-LHC) : Preliminary Design Report. The Large Hadron Collider (LHC) is one of the largest scientific instruments ever built. Since opening up a new energy frontier for exploration in…

Accelerator Physics · Physics 2017-05-29 A. Ballarino , J. P. Burnet , D. Ramos , U. Wagner , S. Weisz , Y. Yang

The Large Hadron Collider (LHC) has been successfully delivering proton-proton collision data at the unprecedented center of mass energy of 13 TeV. An upgrade is planned to increase the instantaneous luminosity delivered by the LHC in what…

Instrumentation and Detectors · Physics 2018-09-10 Peilian Liu

The upgraded Large Hadron Collider beauty (LHCb) experiment is the first detector based at a hadron collider using a fully software based trigger. The first `High Level Trigger' stage (HLT1) reduces the event rate from 30 MHz to…

High Energy Physics - Experiment · Physics 2025-07-25 T. Evans , C. Fitzpatrick , J. Horswill

Decays of b-hadrons are the ideal place to perform measurements of CP violation. Many decay channels allow to over-constrain the unitarity triangles of the CKM matrix and test the SM hypothesis that a single phase is the origin of all CP…

High Energy Physics - Experiment · Physics 2019-08-13 Luca Pescatore

The LHCb detector and LHC running conditions are ideally suited to measuring central exclusive production. Several recent measurements of exclusive dimuon, single and double charmonia are reviewed. The potential for future measurements…

High Energy Physics - Experiment · Physics 2014-09-30 Ronan McNulty

The RICH detectors of the LHCb experiment provide identification of hadrons produced in high energy proton-proton collisions in the LHC at CERN over a wide momentum range (2 to 100 GeV/c). Cherenkov light is collected on photon detector…

Instrumentation and Detectors · Physics 2018-03-14 L. Cassina

The Large Hadron Electron Collider (LHeC) is a proposed upgrade to the LHC, to provide high energy, high luminosity electron-proton collisions to run concurrently with Phase 2 of the LHC. The baseline design of a detector for the LHeC is…

Accelerator Physics · Physics 2013-10-10 Peter Kostka , Alessandro Polini , David M. South

The LHCb experiment collected during run I the world's largest sample of charmed hadrons. This sample is used to search for CP violation in charm and for the measurements of D0 mixing parameters. The measurement of the D0 to D0bar mixing…

High Energy Physics - Experiment · Physics 2019-08-13 Silvia Borghi

Precision measurements of time-integrated CP violation in beauty decays permit a better understanding of the different mechanisms underlying CP violation. They allow to better constrain the Standard Model and probe for new physics. A…

High Energy Physics - Experiment · Physics 2019-05-30 Emilie Bertholet

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

Future Experiments at LHC will have the opportunity to pursue an extensive program on B Physics and CP violation. The expected performance are presented here.

High Energy Physics - Experiment · Physics 2007-05-23 Marta Calvi

Recent results in the field of b and c hadron spectroscopy at the LHCb experiment are presented. The analyses use the data collected with the LHCb detector in proton-proton collisions corresponding to an integrated luminosity up to 3.0…

High Energy Physics - Experiment · Physics 2019-08-13 Ivan Polyakov

The LHCb experiment has fully reconstructed close to 10^9 charm hadron decays---by far the world's largest sample. During the 2011-2012 running periods, the effective proton-proton beam crossing rate was 11-15 MHz while the rate at which…

High Energy Physics - Experiment · Physics 2013-12-03 Patrick Spradlin

The LHCb experiment is a forward spectrometer that offers a unique phase-space coverage at the Large Hadron Collider (LHC). Such a unique coverage offers the possibility to produce complementary and unique physics results in electroweak…

High Energy Physics - Experiment · Physics 2025-06-03 Nathan Grieser

The LHCb experiment is designed for hadronic flavour physics and will look for New Physics manifestations in the decay of charm and bottom hadrons abundantly produced at the LHC. All parts of the LHCb physics programme can be embarked on…

High Energy Physics - Experiment · Physics 2010-10-12 Olivier Schneider

Precision measurements in charm physics offer a window into a unique sector of potential New Physics interactions. LHCb is well equipped to take advantage of the enormous production cross-section of charm mesons in $pp$ collisions at…

High Energy Physics - Experiment · Physics 2019-08-13 S. Borghi

After the observation of a Higgs boson near 125 GeV, the high energy physics community is investigating possible next steps for entering into a new era in particle physics. It is planned that the Large Hadron Collider will deliver an…

High Energy Physics - Phenomenology · Physics 2014-12-31 Altan Cakir