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The Large Hadron-Electron Collider (LHeC) will operate at $\sqrt{s}$ = 1.2 TeV and accumulate about 1/ab of integrated electron-proton luminosity. Novel studies of high energy photon-photon interactions at the LHeC, at the $\gamma\gamma$…

High Energy Physics - Experiment · Physics 2021-09-24 Krzysztof Piotrzkowski , Yuji Yamazaki

The CERN Large Hadron Collider (LHC) is designed to collide proton beams of unprecedented energy, in order to extend the frontiers of high-energy particle physics. During the first very successful running period in 2010--2013, the LHC was…

Based on current CERN infrastructure, an electron--proton collider is proposed at a centre-of-mass energy of about 9 TeV. A 7 TeV LHC bunch is used as the proton driver to create a plasma wakefield which then accelerates electrons to…

High Energy Physics - Experiment · Physics 2016-09-21 A. Caldwell , M. Wing

Under certain running conditions, the CERN Large Hadron Collider (LHC) can be considered as a photon-photon collider. Indeed, in proton-proton, proton-ion, ion-ion collisions, when incoming particles pass very close to each other in very…

High Energy Physics - Phenomenology · Physics 2021-07-28 L. Schoeffel , C. Baldenegro , H. Hamdaoui , S. Hassani , C. Royon , M. Saimpert

The High-Luminosity Large Hadron Collider is expected to deliver up to 3000 fb$^{-1}$ of proton-proton collisions at 14 TeV center-of-mass energy. We present prospects for selected heavy-ion, Standard Model and Higgs sector measurements…

High Energy Physics - Experiment · Physics 2022-08-03 Conor Henderson

Research in cosmic rays is now nearly a century old, but most of the fundamental questions in this field remain unanswered, on the other hand the perspectives of future studies in the next decade are very bright. New detectors will provide…

Astrophysics · Physics 2009-11-07 Paolo Lipari

Based on current CERN infrastructure, an electron-proton collider is proposed at a centre-of-mass energy of about 9 TeV. A 7 TeV LHC bunch is used as the proton driver to create a plasma wakefield which then accelerates electrons to 3 TeV,…

Accelerator Physics · Physics 2015-09-02 Allen Caldwell , Matthew Wing

The proton-proton collisions at the Large Hadron Collider (LHC) produce an intense, high-energy beam of neutrinos of all flavors, collimated in the forward direction. Recently two dedicated neutrino experiments, FASER and SND@LHC, have…

High Energy Physics - Experiment · Physics 2025-01-20 Akitaka Ariga , Jamie Boyd , Felix Kling , Albert De Roeck

A lead scintillator sandwich sampling calorimeter has been installed in the HERA tunnel 105.6 m from the central ZEUS detector in the proton beam direction. It is designed to measure the energy and scattering angle of neutrons produced in…

FASER$\nu$ at the CERN Large Hadron Collider (LHC) is designed to directly detect collider neutrinos for the first time and study their cross sections at TeV energies, where no such measurements currently exist. In 2018, a pilot detector…

The combined zero degree calorimeter (ZDC) is a combination of sampling quartz/tungsten electromagnetic and hadronic calorimeters. Two identical combined calorimeters are located in the LHC tunnel at CERN at the straight section ~140 m on…

Nuclear Experiment · Physics 2019-08-13 O A Grachov , M Murray , J Snyder , J Wood , V Zhukova , A S Ayan , P Debbins , D F Ingram , E Norbeck , Y Onel , E Garcia , G Stephans

We evaluate the performance of an LHCb-like detector using a fast simulation of proton-proton collisions at center-of-mass energies of 50 and 100 TeV. The study shows that detector acceptances and resolutions could be similar to those at…

High Energy Physics - Experiment · Physics 2020-12-07 Veronika Chobanova , Diego Martínez Santos , Claire Prouve , Marcos Romero Lamas

Lepton colliders are considered as options to complement and to extend the physics programme at the Large Hadron Collider. The Compact Linear Collider (CLIC) is an $e^+e^-$ collider under development aiming at centre-of-mass energies of up…

Instrumentation and Detectors · Physics 2014-01-14 C. Adloff , J. -J. Blaising , M. Chefdeville , C. Drancourt , R. Gaglione , N. Geffroy , Y. Karyotakis , I. Koletsou , J. Prast , G. Vouters , J. Repond , J. Schlereth , J. Smith , L. Xia , E. Baldolemar , J. Li , S. T. Park , M. Sosebee , A. P. White , J. Yu , G. Eigen , M. A. Thomson , D. R. Ward , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , D. Dannheim , A. Dotti , K. Elsener , G. Folger , C. Grefe , V. Ivantchenko , M. Killenberg , W. Klempt , E. van der Kraaij , C. B. Lam , L. Linssen , A. -I. Lucaci-Timoce , A. Muennich , S. Poss , A. Ribon , A. Sailer , D. Schlatter , J. Strube , V. Uzhinskiy , C. Carloganu , P. Gay , S. Manen , L. Royer , M. Tytgat , N. Zaganidis , G. C. Blazey , A. Dyshkant , J. G. R. Lima , V. Zutshi , J. -Y. Hostachy , L. Morin , U. Cornett , D. David , A. Ebrahimi , G. Falley , N. Feege , K. Gadow , P. Goettlicher , C. Guenter , O. Hartbrich , B. Hermberg , S. Karstensen , F. Krivan , K. Krueger , S. Lu , B. Lutz , S. Morozov , V. Morgunov , C. Neubueser , M. Reinecke , F. Sefkow , P. Smirnov , M. Terwort , E. Garutti , S. Laurien , I. Marchesini , M. Matysek , M. Ramilli , K. Briggl , P. Eckert , T. Harion , H. -Ch. Schultz-Coulon , W. Shen , R. Stamen , B. Bilki , E. Norbeck , D. Northacker , Y. Onel , G. W. Wilson , K. Kawagoe , Y. Sudo , T. Yoshioka , P. D. Dauncey , M. Wing , F. Salvatore , E. Cortina Gil , S. Mannai , G. Baulieu , P. Calabria , L. Caponetto , C. Combaret , R. Della Negra , G. Grenier , R. Han , J-C. Ianigro , R. Kieffer , I. Laktineh , N. Lumb , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , W. Tromeur , M. Vander Donckt , Y. Zoccarato , E. Calvo Alamillo , M. -C. Fouz , J. Puerta-Pelayo , F. Corriveau , B. Bobchenko , M. Chadeeva , M. Danilov , A. Epifantsev , O. Markin , R. Mizuk , E. Novikov , V. Popov , V. Rusinov , E. Tarkovsky , N. Kirikova , V. Kozlov , P. Smirnov , Y. Soloviev , D. Besson , P. Buzhan , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , V. Tikhomirov , C. Kiesling , K. Seidel , F. Simon , C. Soldner , M. Szalay , M. Tesar , L. Weuste , M. S. Amjad , J. Bonis , S. Callier , S. Conforti di Lorenzo , P. Cornebise , Ph. Doublet , F. Dulucq , J. Fleury , T. Frisson , N. van der Kolk , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , J. Rouene , N. Seguin-Moreau , M. Anduze , V. Balagura , V. Boudry , J-C. Brient , R. Cornat , M. Frotin , F. Gastaldi , E. Guliyev , Y. Haddad , F. Magniette , G. Musat , M. Ruan , T. H. Tran , H. Videau , B. Bulanek , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , D. Lednicky , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , B. Belhorma , H. Ghazlane , K. Kotera , T. Takeshita , S. Uozumi , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , M. Goetze , J. Sauer , S. Weber , C. Zeitnitz

The differential cross section for inclusive particle production as a function of energy in proton-proton collisions at a center-of-mass energy of 13 TeV is measured in the very forward region of the CMS detector. The measurement is based…

High Energy Physics - Experiment · Physics 2017-08-16 CMS Collaboration

The LHCb experiment has the unique possibility, among the LHC experiments, to be operated in fixed target mode, using its internal gas target. The energy scale achievable at the LHC, combined with the LHCb forward geometry and detector…

High Energy Physics - Experiment · Physics 2017-05-17 Giacomo Graziani

The future proton-proton collider (FCC-hh) will deliver collisions at a center of mass energy up to $\sqrt{s}=100$ TeV at an unprecedented instantaneous luminosity of $L=3~10^{35}$ cm$^{-2}$s$^{-1}$, resulting in extremely challenging…

The identification of gamma-ray induced air showers with Cherenkov telescopes suffers from contamination with a specific class of cosmic ray induced air showers. The predictions for this background show strong discrepancies between the…

High Energy Physics - Phenomenology · Physics 2025-03-25 Clara E. Leitgeb , Robert D. Parsons , Andrew Taylor , Kenneth Ragan , David Berge , Cigdem Issever

The current large uncertainty on the extrapolation of the proton-proton total cross section at the LHC energy will be resolved by the precise measurement by the TOTEM experiment. Its accurate studies on the basic properties of proton-proton…

High Energy Physics - Experiment · Physics 2008-11-26 Stefano Lami

The performance is presented of the reconstruction and identification algorithms for electrons and photons with the CMS experiment at the LHC. The reported results are based on proton-proton collision data collected at a center-of-mass…

High Energy Physics - Experiment · Physics 2021-05-19 CMS Collaboration

Experiments at particle colliders have reached center of mass energies well above 100 GeV, equivalent to temperatures which existed shortly after the big bang. These experiments, testing the initial conditions of the universe have, with…

High Energy Physics - Experiment · Physics 2009-09-25 M. Dittmar