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High-energy physics experiments face extreme data rates, requiring real-time trigger systems to reduce event throughput while preserving sensitivity to rare processes. Trigger systems are typically constructed as modular chains of…

High Energy Physics - Experiment · Physics 2026-03-10 Noah Clarke Hall , Ioannis Xiotidis , Nikos Konstantinidis , David W. Miller

The ALICE Experiment has replaced its Inner Tracking System with a 7-layer pixel-only tracker made out of more than 24000 monolithic active pixel sensor chips, in order to fulfill the requirements of the physics program of the LHC Run 3.…

Instrumentation and Detectors · Physics 2023-02-02 Andrea Sofia Triolo

The ATLAS experiment has successfully recorded over 300 nb^-1 of pp collisions at 7 TeV provided by the Large Hadron Collider, with an efficiency of 94%. We describe the data acquisition, trigger, reconstruction, calibration, monitoring,…

Instrumentation and Detectors · Physics 2019-08-13 Peter Onyisi

Searches for long-lived particles (LLPs) are among the most promising avenues for discovering physics beyond the Standard Model at the Large Hadron Collider (LHC). However, displaced signatures are notoriously difficult to identify due to…

High Energy Physics - Experiment · Physics 2023-12-14 ATLAS Collaboration

The ATLAS experiment has been taking data efficiently since LHC collisions started, first at the injection energy of 450 GeV/beam and at 1.18 TeV/beam in 2009, then at 3.5 TeV/beam in 2010. Many results have already been obtained based on…

High Energy Physics - Experiment · Physics 2019-08-14 Thorsten Wengler

The central detectors of the ALICE experiment at LHC will produce a data size of up to 75 MByte/event at an event rate <200 Hz resulting in a data rate of \~15 GByte/sec. This exceeds the foreseen mass storage bandwidth of 1.25 GByte/sec by…

Instrumentation and Detectors · Physics 2016-09-08 Anders Vestbo

Multiple proton-proton collisions (pile-up) occur at every bunch crossing at the LHC, with the mean number of interactions expected to reach 80 during Run 3 and up to 200 at the High-Luminosity LHC. As a direct consequence, events with…

High Energy Physics - Experiment · Physics 2025-12-12 Mohammed Aboelela

The trigger system of the LHCb experiment is discussed in this paper and its performance is evaluated on a dataset recorded during the 2012 run of the LHC. The main purpose of the LHCb trigger system is to separate heavy flavour signals…

High Energy Physics - Experiment · Physics 2014-06-13 J. Albrecht , V. V. Gligorov , G. Raven , S. Tolk

Radiation damage significantly impacts the performance of silicon tracking detectors in Large Hadron Collider (LHC) experiments such as ATLAS and CMS, with signal reduction being the most critical effect. Adjusting sensor bias voltage and…

High Energy Physics - Experiment · Physics 2025-01-22 Marco Bomben , Keerthi Nakkalil

The new Inner Tracking System (ITS2) of the ALICE experiment began operation in 2021 with the start of LHC Run 3. Compared to its predecessor, ITS2 offers substantial improvements in pointing resolution, tracking efficiency at low…

Instrumentation and Detectors · Physics 2026-04-15 D. Agguiaro , G. Aglieri Rinella , L. Aglietta , M. Agnello , F. Agnese , B. Alessandro , G. Alfarone , J. Alme , E. Anderssen , D. Andreou , M. Angeletti , N. Apadula , P. Atkinson , C. Azzan , R. Baccomi , A. Badalà , A. Balbino , P. Barberis , F. Barile , L. Barioglio , R. Barthel , F. Baruffaldi , N. K. Behera , I. Belikov , A. Benato , M. Benettoni , F. Benotto , S. Beole , N. Bez , A. Bhatti , M. Bhopal , A. P. Bigot , G. Boca , G. Bonomi , M. Bonora , F. Borotto Dalla Vecchia , M. Borri , V. Borshchov , E. Botta , L. Boynton , G. Brower , E. Bruna , O. Brunasso Cattarello , G. E. Bruno , M. D. Buckland , S. Bufalino , P. Camerini , P. Cariola , C. Ceballos Sanchez , J. Cho , S. Cho , K. Choi , Y. Choi , N. J. Clague , O. A. Clausse , F. Colamaria , D. Colella , S. Coli , A. Collu , M. Concas , G. Contin , Y. Corrales Morales , S. Costanza , J. B. Dainton , E. Danè , W. Degraw , C. De Martin , W. Deng , G. De Robertis , P. Dhankher , A. Di Mauro , F. Dumitrache , D. Elia , M. R. Ersdal , J. Eum , A. Fantoni , G. Feofilov , J. Ferencei , F. Fichera , G. Fiorenza , A. N. Flores , A. Franco , M. Franco , J. P. Fransen , D. Gajanana , A. Galdames Perez , C. Gao , C. Gargiulo , L. Garizzo , P. Giubilato , M. Goffe , A. Grant , E. Grecka , L. Greiner , A. Grelli , A. Grimaldi , O. S. Groettvik , F. Grosa , C. Guo Hu , R. P. Hannigan , H. Helstrup , A. Hill , H. Hillemanns , P. Hindley , G. Huang , M. Iannone , J. P. Iddon , P. Ijzermans , M. A. Imhoff , A. Isakov , J. Jeong , T. Johnson , A. Junique , J. Kaewjai , M. Keil , Z. Khabanova , H. Khan , H. Kim , J. Kim , J. Kim , J. Kim , M. Kim , T. Kim , J. Klein , C. Kobdaj , A. Kotliarov , M. J. Kraan , I. Králik , F. Krizek , T. Kugathasan , C. Kuhn , P. G. Kuijer , S. Kushpil , M. J. Kweon , M. Kwon , Y. Kwon , P. La Rocca , N. Lacalamita , P. Larionov , G. Ledey , S. Lee , T. Lee , R. C. Lemmon , Y. Lesenechal , E. D. Lesser , B. E. Liang-Gilman , F. Librizzi , B. Lim , S. Lim , S. Lindsay , J. Liu , J. Liu , F. Loddo , M. Lupi , M. Mager , A. Maire , G. Mandaglio , V. Manzari , C. Markert , G. Markey , D. Marras , P. Martinengo , S. Martiradonna , M. Masera , A. Mastroserio , G. Mazza , D. Mazzaro , F. Mazzaschi , M. Mazzilli , L. Mcalpine , M. Mongelli , J. Morant , F. Morel , P. Morrall , V. Muccifora , A. Mulliri , L. Musa , A. I. Nambrath , M. Obergger , A. Orlandi , A. Palasciano , R. Panero , E. Paoletti , G. S. Pappalardo , O. Parasole , J. Park , L. Passamonti , C. Pastore , R. N. Patra , F. Pellegrino , A. Pepato , C. Petta , S. Piano , D. Pierluigi , S. Pisano , M. Pĺoskoń , M. T. Poblocki , S. Politano , E. Prakasa , F. Prino , M. Protsenko , M. Puccio , C. Puggioni , A. Rachevski , L. Ramello , M. Rasa , I. Ravasenga , A. U. Rehman , F. Reidt , M. Richter , F. Riggi , M. Rizzi , K. Røed , D. Röhrich , F. Ronchetti , M. J. Rossewij , A. Rossi , A. Russo , B. Di Ruzza , G. Saccà , M. Sacchetti , R. Sadikin , A. Sanchez Gonzalez , U. Savino , J. Schambach , F. Schlepper , R. Schotter , P. J. Secouet , M. Selina , S. Senyukov , J. J. Seo , R. Shahoyan , S. Shaukat , F. Shirokopetlev , K. Sielewicz , G. Simantovic , M. Sitta , R. J. M. Snellings , W. Snoeys , J. Song , J. M. Sonneveld , R. Spijkers , A. Sturniolo , C. P. Stylianidis , M. Šuljić , D. Sun , X. Sun , R. A. Syed , A. Szczepankiewicz , C. Terrevoli , M. Toppi , A. Trifiró , A. S. Triolo , S. Trogolo , V. Trubnikov , M. Turcato , R. Turrisi , T. Tveter , I. Tymchuk , G. L. Usai , V. Valentino , N. Valle , J. B. Van Beelen , J. W. Van Hoorne , T. Vanat , M. Varga-Kofarago , A. Velure , G. Venier , F. Veronese , A. Villani , A. Viticchié , C. Wabnitz , Y. Wang , P. Yang , E. R. Yeats , I. -K. Yoo , J. H. Yoon , S. Yuan , V. Zaccolo , A. Zampieri , C. Zampolli , E. Zhang , L. Zhang , X. Zhang , Z. Zhang , V. Zherebchevskii , N. Zurlo

In LHC Run 3, ALICE will increase the data taking rate significantly to 50 kHz continuous readout of minimum bias Pb--Pb collisions. The reconstruction strategy of the online-offline computing upgrade foresees a first synchronous online…

Instrumentation and Detectors · Physics 2020-09-17 David Rohr

To meet the demands of the Beam Energy Scan phase-II (BES-II) program, the STAR experiment at RHIC developed a dual real-time framework consisting of a High Level Trigger (HLT) and an Express Data Production system (xProduction). The HLT…

The ATLAS experiment at the Large Hadron Collider (LHC) has been able to collect 5.25 fb-1 of data in 2011. For many physics analyses both in context of the Standard Model (SM) and Beyond the Standard Model (BSM) theories such as Higgs…

High Energy Physics - Experiment · Physics 2015-06-03 Marcus M. Morgenstern

Circular collider designs are tailored to maximise luminosity delivered to experimental detectors, effectively utilising the charged beams that have been accelerated for collisions. In reality, the key metric for the effective operation of…

Accelerator Physics · Physics 2025-04-18 F. Capoani , A. Bazzani , B. Giacobbe , M. Giovannozzi

The Pixel Detector is the innermost detector of the tracking system of the Compact Muon Solenoid (CMS) experiment at CERN Large Hadron Collider (LHC). It precisely determines the interaction point (primary vertex) of the events and the…

Instrumentation and Detectors · Physics 2015-10-14 Chang-Seong Moon , Aurore Savoy-Navarro

Collider experiments are equipped with trigger systems that rapidly inspect the physics content emerging from collisions to decide whether the resulting products are worth saving for later analysis. One crucial aspect for analyzing the…

High Energy Physics - Experiment · Physics 2026-04-14 Andrea Coccaro , Carlo Schiavi , Alessandro Zaio

Real-time data filtering and selection -- or trigger -- systems at high-throughput scientific facilities such as the experiments at the Large Hadron Collider (LHC) must process extremely high-rate data streams under stringent bandwidth,…

The ATLAS experiment will undergo around the year 2025 a replacement of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) with a new 5-layer pixel system. Thin planar pixel sensors are promising candidates to…

Instrumentation and Detectors · Physics 2017-02-01 Anna Macchiolo , Julien Beyer , Alessandro La Rosa , Richard Nisius , Natascha Savic

The Muon Spectrometer (MS) of the ALICE experiment at LHC is equipped with a HLT (High Level Trigger), whose aim is to improve the accuracy of the trigger cuts delivered at the L0 stage. A computational challenge of real-time event…

Instrumentation and Detectors · Physics 2015-03-19 Indranil Das

At the Large Hadron Collider (LHC), the trigger systems for the detectors must be able to process a very large amount of data in a very limited amount of time, so that the nominal collision rate of 40 MHz can be reduced to a data rate that…

Instrumentation and Detectors · Physics 2015-06-17 P. Lujan , V. Halyo , A. Hunt , P. Jindal , P. LeGresley