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Related papers: The first-level trigger of ATLAS

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Measurements are presented from proton-proton collisions at centre-of-mass energies of sqrt(s) = 0.9, 2.36 and 7 TeV recorded with the ATLAS detector at the LHC. Events were collected using a single-arm minimum-bias trigger. The…

High Energy Physics - Experiment · Physics 2015-03-17 The ATLAS Collaboration

The high-luminosity phase of the Large Hadron Collider will provide 5-7 times greater luminosities than assumed in the original detector design. An improved trigger system requires an upgrade of the readout electronics of the ATLAS Liquid…

Instrumentation and Detectors · Physics 2020-09-16 Tiankuan Liu

The expected performance of the ATLAS and CMS detectors at the Large Hadron Collider (LHC) in QCD and top quark measurements is discussed, with a focus on the early data taking phase. Such processes are amongst the primary backgrounds in…

High Energy Physics - Experiment · Physics 2014-11-18 Frank-Peter Schilling

A study on the use of a machine learning algorithm for the level 1 trigger decision in the JUNO experiment ispresented. JUNO is a medium baseline neutrino experiment in construction in China, with the main goal of determining the neutrino…

Instrumentation and Detectors · Physics 2021-09-01 Barbara Clerbaux , Pierre-Alexandre Petitjean , Yu Xu , Yifan Yang

We summarize the analysis of high-pT jets in early pp collisions recorded with the ATLAS detector. Two searches for new physics are presented: One for dijet resonances, and one for quark contact interactions. The first search sets the most…

High Energy Physics - Experiment · Physics 2019-08-13 Georgios Choudalakis

We present first measurements of charged and neutral particle-flow correlations in pp collisions using the ATLAS calorimeters. Data were collected in 2009 and 2010 at centre-of-mass energies of 900 GeV and 7 TeV. Events were selected using…

High Energy Physics - Experiment · Physics 2012-08-27 The ATLAS Collaboration

The LHCb experiment at CERN is undergoing an upgrade in preparation for the Run 3 data taking period of the LHC. As part of this upgrade the trigger is moving to a fully software implementation operating at the LHC bunch crossing rate. We…

Instrumentation and Detectors · Physics 2022-01-06 R. Aaij , M. Adinolfi , S. Aiola , S. Akar , J. Albrecht , M. Alexander , S. Amato , Y. Amhis , F. Archilli , M. Bala , G. Bassi , L. Bian , M. P. Blago , T. Boettcher , A. Boldyrev , S. Borghi , A. Brea Rodriguez , L. Calefice , M. Calvo Gomez , D. H. Cámpora Pérez , A. Cardini , M. Cattaneo , V. Chobanova , G. Ciezarek , X. Cid Vidal , J. L. Cobbledick , J. A. B. Coelho , T. Colombo , A. Contu , B. Couturier , D. C. Craik , R. Currie , P. d'Argent , M. De Cian , D. Derkach , F. Dordei , M. Dorigo , L. Dufour , P. Durante , A. Dziurda , A. Dzyuba , S. Easo , S. Esen , P. Fernandez Declara , S. Filippov , C. Fitzpatrick , M. Frank , P. Gandini , V. V. Gligorov , E. Golobardes , G. Graziani , L. Grillo , P. A. Günther , S. Hansmann-Menzemer , A. M. Hennequin , L. Henry , D. Hill , S. E. Hollitt , J. Hu , W. Hulsbergen , R. J. Hunter , M. Hushchyn , B. K. Jashal , C. R. Jones , S. Klaver , K. Klimaszewski , R. Kopecna , W. Krzemien , M. Kucharczyk , R. Lane , F. Lazzari , R. Le Gac , P. Li , J. H. Lopes , M. Lucio Martinez , A. Lupato , O. Lupton , X. Lyu , F. Machefert , O. Madejczyk , S. Malde , J. F. Marchand , S. Mariani , C. Marin Benito , D. Martinez Santos , F. Martinez Vidal , R. Matev , M. Mazurek , B. Mitreska , D. S. Mitzel , M. J. Morello , H. Mu , P. Muzzetto , P. Naik , M. Needham , N. Neri , N. Neufeld , N. S. Nolte , D. O'Hanlon , A. Oyanguren , M. Pepe Altarelli , S. Petrucci , M. Petruzzo , L. Pica , F. Pisani , A. Piucci , F. Polci , A. Poluektov , E. Polycarpo , C. Prouve , G. Punzi , R. Quagliani , R. I. Rabadan Trejo , M. Ramos Pernas , M. S. Rangel , F. Ratnikov , G. Raven , F. Reiss , V. Renaudin , P. Robbe , A. Ryzhikov , M. Santimaria , M. Saur , M. Schiller , R. Schwemmer , B. Sciascia , A. Solomin , F. Suljik , N. Skidmore , M. D. Sokoloff , P. Spradlin , M. Stahl , S. Stahl , H. Stevens , L. Sun , A. Szabelski , T. Szumlak , M. Szymanski , D. Y. Tou , G. Tuci , A. Usachov , N. Valls Canudas , R. Vazquez Gomez , S. Vecchi , M. Vesterinen , X. Vilasis-Cardona , D. Vom Bruch , Z. Wang , T. Wojton , M. Whitehead , M. Williams , M. Witek , Y. Xie , A. Xu , H. Yin , M. Zdybal , O. Zenaiev , D. Zhang , L. Zhang , X. Zhu

This paper presents several component prototypes towards a low-latency, small-form-factor optical link designed for the ATLAS Liquid Argon Calorimeter Phase-I trigger upgrade. A prototype of the custom-made dual-channel optical transmitter…

After 2001 the upgraded ep collider HERA will provide an about five times higher luminosity for the two experiments H1 and ZEUS. In order to cope with the expected higher event rates the H1 collaboration is building a track based trigger…

High Energy Physics - Experiment · Physics 2014-11-17 A. Baird , E. Elsen , Y. H. Fleming , M. Kolander , S. Kolya , D. Meer , D. Mercer , J. Naumann , P. R. Newman , D. Sankey , A. Schoening , H. -C. Schultz-Coulon , Ch. Wissing

The Large Hadron Collider (LHC) will provide a huge amount of top-antitop events, making the LHC a top quark factory, producing 1 tt pair per second at a luminosity of 10^33cm-2s-1. A large top quark sample will be available from the start…

High Energy Physics - Experiment · Physics 2019-08-14 M. Vander Donckt

The ATLAS experiment at the Large Hadron Collider has a broad physics programme ranging from precision measurements to direct searches for new particles and new interactions, requiring ever larger and ever more accurate datasets of…

High Energy Physics - Experiment · Physics 2024-11-25 ATLAS Collaboration

The reconstruction of the signal from hadrons and jets emerging from the proton-proton collisions at the Large Hadron Collider (LHC) and entering the ATLAS calorimeters is based on a three-dimensional topological clustering of individual…

High Energy Physics - Experiment · Physics 2017-08-24 ATLAS Collaboration

The SuperCDMS SNOLAB dark matter search experiment aims to be sensitive to energy depositions down to O(1 eV). This imposes requirements on the resolution, signal efficiency, and noise rejection of the trigger system. To accomplish this,…

The Large Hadron Collider (LHC) at CERN will provide proton-proton collisions at a centre-of-mass energy of 14 TeV with a design luminosity of 10**34/cm**2/s. The exploitation of the rich physics potential offered by the LHC will be…

High Energy Physics - Experiment · Physics 2007-05-23 Felicitas Pauss , Michael Dittmar

Many theoretical models, like the Standard Model or SUSY at large tan(beta), predict Higgs bosons or new particles which decay more abundantly to final states including tau leptons than to other leptons. At the energy scale of the LHC, the…

After the successful LHC operation at the center-of-mass energies of 7 and 8 TeV in 2010-2012, plans are actively advancing for a series of upgrades of the accelerator, culminating roughly ten years from now in the high-luminosity LHC…

Instrumentation and Detectors · Physics 2014-08-29 Walter Hopkins

The LHC will undergo a major upgrade starting in 2025 towards the High Luminosity LHC (HL-LHC) to increase the instantaneous luminosity by a factor of 5 to 7 compared to the nominal value. The Phase-II Upgrade (2025-2027) will require the…

Instrumentation and Detectors · Physics 2020-11-06 Fernando Carrió Argos

The ALICE (A Large Ion Collider Experiment) detector yields a huge sample of data from different sub-detectors. On-line data processing is applied to select and reduce the volume of the stored data. ALICE applies a multi-level hardware…

Instrumentation and Detectors · Physics 2019-08-14 F. Ronchetti , F. Blanco , M. Figueredo , A. G. Knospe , L. Xaplanteris

A summary of some of the recent minimum bias and underlying event measurements by the ATLAS collaboration is given. The results of several analyses using low-luminosity proton-proton collision data from the LHC taken at center-of-mass…

High Energy Physics - Experiment · Physics 2019-08-13 Michael Leyton

In planning for the Phase II upgrades of CMS and ATLAS major considerations are: 1)being able to deal with degradation of tracking and calorimetry up to the radiation doses to be expected with an integrated luminosity of 3000 $fb^{-1}$ and…

Instrumentation and Detectors · Physics 2013-10-08 Sebastian White
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