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The CMS experiment has been designed with a two-level trigger system: the Level-1 Trigger, implemented on custom-designed electronics, and the High Level Trigger, a streamlined version of the CMS offline reconstruction software running on a…

Instrumentation and Detectors · Physics 2020-11-19 Thiago R. F. P. Tomei

Increasing luminosity at the Fermilab Tevatron collider has led the D0 collaboration to make improvements to its detector beyond those already in place for Run IIa, which began in March 2001. One of the cornerstones of this Run IIb upgrade…

Instrumentation and Detectors · Physics 2008-11-26 M. Abolins

The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then…

Instrumentation and Detectors · Physics 2020-12-30 ATLAS Collaboration

The CMS experiment at the LHC has started data taking in Run 3 at a $\mathrm{pp}$ collision energy of $13.6~\mathrm{TeV}$. In preparation for Run 3, detector systems, such as Pixel Tracker, HCAL and CSC, have been upgraded due to…

High Energy Physics - Experiment · Physics 2023-09-07 Srećko Morović

The first level trigger of the CMS experiment is comprised of custom electronics that process data from the electromagnetic and hadron calorimeters and three technologies of muon detectors in order to select the most interesting events from…

High Energy Physics - Experiment · Physics 2019-08-13 J. Brooke

The High-Luminosity LHC (HL-LHC) will usher in a new era in high-energy physics. The HL-LHC experimental conditions entail an instantaneous luminosity of up to $7.5 \times 10^{34}$ cm$^{-2}$ s$^{-1}$ and up to 200 simultaneous collisions…

High Energy Physics - Experiment · Physics 2022-11-17 Thiago R. F. P. Tomei

As the Tevatron luminosity increases sophisticated selections are required to be efficient in selecting rare events among a very huge background. To cope with this problem, CDF has pushed the offline calorimeter algorithm reconstruction…

Instrumentation and Detectors · Physics 2008-10-22 A. Canepa , M. Casarsa , T. Liu , G. Cortiana , G. Flanagan , H. Frisch , D. Krop , C. Pilcher , V. Rusu , V. Cavaliere , V. Greco , P. Giannetti , M. Piendibene , L. Sartori , M. Vidal

This paper describes the CMS trigger system and its performance during Run 1 of the LHC. The trigger system consists of two levels designed to select events of potential physics interest from a GHz (MHz) interaction rate of proton-proton…

Instrumentation and Detectors · Physics 2017-01-26 CMS Collaboration

The trigger systems of the CERN LHC detectors play a crucial role in determining the physics capabilities of the experiments. A reduction of several orders of magnitude of the event rate is needed to reach values compatible with the…

Instrumentation and Detectors · Physics 2014-09-18 Juliette Alimena

At the start of Run 2 in 2015, the LHC delivered proton-proton collisions at a center-of-mass energy of 13 TeV. During Run 2 (years 2015-2018) the LHC eventually reached a luminosity of 2.1 $\times$ 10$^{34}$ cm$^{-2}$ s$^{-1}$, almost…

High Energy Physics - Experiment · Physics 2020-10-21 CMS Collaboration

The ATLAS trigger has been used very successfully for the online event selection during the first part of the second LHC run (Run-2) in 2015/16 at a center-of-mass energy of 13 TeV. The trigger system is composed of a hardware Level-1…

High Energy Physics - Experiment · Physics 2019-08-13 Catrin Bernius

The CMS Electromagnetic Calorimeter (ECAL) is a high resolution crystal calorimeter operating at the CERN LHC. It is responsible for the identification and precise reconstruction of electrons and photons in CMS, which were crucial in the…

Instrumentation and Detectors · Physics 2019-10-15 Abraham Tishelman-Charny

The Phase-I trigger readout electronics upgrade of the ATLAS Liquid Argon calorimeters enhances the physics reach of the experiment during the upcoming operation at increasing Large Hadron Collider luminosities. The new system, installed…

Instrumentation and Detectors · Physics 2022-05-17 G. Aad , A. V. Akimov , K. Al Khoury , M. Aleksa , T. Andeen , C. Anelli , N. Aranzabal , C. Armijo , A. Bagulia , J. Ban , T. Barillari , F. Bellachia , M. Benoit , F. Bernon , A. Berthold , H. Bervas , D. Besin , A. Betti , Y. Bianga , M. Biaut , D. Boline , J. Boudreau , T. Bouedo , N. Braam , M. Cano Bret , G. Brooijmans , H. Cai , C. Camincher , A. Camplani , S. Cap , A. Carbone , J. W. S. Carter , S. V. Chekulaev , H. Chen , K. Chen , N. Chevillot , M. Citterio , B. Cleland , M. Constable , S. de Jong , A. M. Deiana , M. Delmastro , B. Deng , H. Deschamps , C. Diaconu , A. Dik , B. Dinkespiler , N. Dumont Dayot , A. Emerman , Y. Enari , P. J. Falke , J. Farrell , W. Fielitz , E. Fortin , J. Fragnaud , S. Franchino , L. Gantel , K. Gigliotti , D. Gong , A. Grabas , P. Grohs , N. Guettouche , T. Guillemin , D. Guo , J. Guo , L. Hasley , C. Hayes , R. Hentges , L. Hervas , M. Hils , J. Hobbs , A. Hoffman , D. Hoffmann , P. Horn , T. Hryn'ova , L. Iconomidou-Fayard , R. Iguchi , T. James , K. Johns , T. Junkermann , C. Kahra , E. F. Kay , R. Keeler , S. Ketabchi Haghighat , P. Kinget , E. Knoops , A. Kolbasin , P. Krieger , J. Kuppambatti , L. L. Kurchaninov , E. Ladygin , S. Lafrasse , M. P. J. Landon , F. Lanni , S. Latorre , D. Laugier , M. Lazzaroni , X. Le , P. Le Bourlout , C. A. Lee , M. Lefebvre , M. A. L. Leite , C. Leroy , X. Li , Z. Li , F. Liang , H. Liu , C. Liu , T. Liu , H. Ma , L. L. Ma , D. J. Mahon , U. Mallik , B. Mansoulie , A. L. Maslennikov , N. Matsuzawa , R. A. McPherson , S. Menke , A. Milic , Y. Minami , E. Molina , E. Monnier , N. Morange , L. Morvaj , J. Mueller , C. Mwewa , R. Narayan , N. Nikiforou , I. Ochoa , R. Oishi , D. Oliveira Damazio , R. E. Owen , C. Pancake , D. K. Panchal , G. Perrot , M. -A. Pleier , P. Poffenberger , R. Porter , S. Quan , J. Rabel , A. Roy , J. P. Rutherfoord , F. Sabatini , F. Salomon , E. Sauvan , A. C. Schaffer , R. D. Schamberger , Ph. Schwemling , C. Secord , L. Selem , K. Sexton , E. Shafto , M. V. Silva Oliveira , S. Simion , S. Singh , W. Sippach , A. A. Snesarev , S. Snyder , M. Spalla , S. Stärz , A. Straessner , P. Strizenec , R. Stroynowski , V. V. Sulin , J. Tanaka , S. Tang , S. Tapprogge , G. F. Tartarelli , G. Tateno , K. Terashi , S. Tisserant , D. Tompkins , G. Unal , M. Unal , K. Uno , A. Vallier , S. Vieira de Souza , R. Walker , Q. Wang , C. Wang , R. Wang , M. Wessels , I. Wingerter-Seez , K. Wolniewicz , W. Wu , Z. Xiandong , R. Xu , H. Xu , S. Yamamoto , Y. Yang , J. Ye , H. Zaghia , J. Zang , T. Zhang , H. L. Zhu , V. Zhulanov , E. Zonca , G. Zuk

During LHC Run 2 (2015-2018) the ATLAS Level-1 topological trigger allowed efficient data-taking by the ATLAS experiment at luminosities up to 2.1x10$^{34}$ cm$^{-2}$s$^{-1}$, which exceeds the design value by a factor of two. The system…

High Energy Physics - Experiment · Physics 2022-01-14 ATLAS Collaboration

The Level-1 trigger of the CMS experiment at CERN has been designed to select proton-proton interactions whose final state includes signatures of new physics in the form of high transverse energy electrons, photons, jets, or high missing…

Instrumentation and Detectors · Physics 2008-10-23 C. Foudas

The calibration and performance of the LHCb Calorimeter system in Run 1 and 2 at the LHC are described. After a brief description of the sub-detectors and of their role in the trigger, the calibration methods used for each part of the…

The CMS experiment will collect data from the proton-proton collisions delivered by the Large Hadron Collider (LHC) at a centre-of-mass energy up to 14 TeV. The CMS trigger system is designed to cope with unprecedented luminosities and LHC…

Instrumentation and Detectors · Physics 2009-05-07 Marta Felcini , Marco Zanetti

The CMS experiment has been designed with a 2-level trigger system: the Level 1 Trigger, implemented on custom-designed electronics, and the High Level Trigger (HLT), a streamlined version of the CMS offline reconstruction software running…

Instrumentation and Detectors · Physics 2015-06-19 Valentina Gori

An efficient and precise reconstruction of charged-particle tracks is crucial for the overall performance of the CMS experiment. During Run 2 of LHC, significant upgrades were made to the track reconstruction algorithms in order to…

Instrumentation and Detectors · Physics 2020-12-15 Walaa Elmetenawee

After the current shutdown, the LHC is about to resume operation for a new data-taking period, when it will operate with increased luminosity, event rate and center of mass energy. The new conditions will impose more demanding constraints…

Instrumentation and Detectors · Physics 2019-08-13 Sebastien Prince
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