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A detector designed to measure early particle showers has been installed in front of the central CDF calorimeter at the Tevatron. This new preshower detector is based on scintillator tiles coupled to wavelength-shifting fibers read out by…

Instrumentation and Detectors · Physics 2014-11-18 Michele Gallinaro

An improved weighting algorithm applied to hadron showers has been developed for a fine grained LAr calorimeter. The new method uses tabulated weights which depend on the density of energy deposited in individual cells and in a surrounding…

Instrumentation and Detectors · Physics 2009-11-10 C. Issever , K. Borras , D. Wegener

This paper describes the implementation and performance of a particle flow algorithm applied to 20.2 fb$^{-1}$ of ATLAS data from 8 TeV proton-proton collisions in Run 1 of the LHC. The algorithm removes calorimeter energy deposits due to…

High Energy Physics - Experiment · Physics 2017-08-15 ATLAS Collaboration

We present measurements of the top-antitop production cross section in b-tagged lepton + jets events from proton-antiproton collisions at 1.96 TeV using the CDF detector at Fermilab. B-jets are tagged with either a secondary vertex…

High Energy Physics - Experiment · Physics 2010-11-05 Henri Bachacou

The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10000 photomultipliers collect light from scintillating tiles acting as the active material…

High Energy Physics - Experiment · Physics 2018-12-07 ATLAS Collaboration

An assessment of the recorded integrated luminosity is presented for data collected with the D0 detector at the Fermilab Tevatron Collider from June 2006 to September 2011 (Run IIb). In addition, a measurement of the effective cross section…

The ATLAS Trigger system is a key component of the ATLAS experiment at the CERN Large Hadron Collider (LHC), designed to reduce the event rate from the 40 MHz proton-proton bunch crossing frequency to an output suitable for offline storage…

Instrumentation and Detectors · Physics 2026-03-17 Leonardo Toffolin

We present results of a search for for the anomalous production of events containing a high-transverse momentum charged lepton (electron or muon) and photon, accompanied by missing transverse energy (MET), and/or additional leptons and…

High Energy Physics - Experiment · Physics 2009-09-29 A. Loginov

An optical link system is being developed for the ATLAS Liquid Argon Calorimeter Phase-II upgrade. The optical link system is responsible for transmit the data of over 182 thousand detector channels from 1524 Front-End Boards (FEBs) through…

Instrumentation and Detectors · Physics 2020-08-03 B. Deng , C. Liu , D. Gong , X. Huang , S. Hou , T. Liu , H. Sun , L. Zhang , W. Zhang , J. Ye

The CMS experiment at the CERN LHC will be upgraded to accommodate the 5-fold increase in the instantaneous luminosity expected at the High-Luminosity LHC (HL-LHC). Concomitant with this increase will be an increase in the number of…

Instrumentation and Detectors · Physics 2021-04-28 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , M. Alhusseini , J. Alison , G. Altopp , M. Alyari , S. An , S. Anagul , I. Andreev , M. Andrews , P. Aspell , I. A. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , P. Bargassa , D. Barney , E. Becheva , P. Behera , A. Belloni , T. Bergauer , M. Besancon , S. Bhattacharya , S. Bhattacharya , D. Bhowmik , P. Bloch , A. Bodek , M. Bonanomi , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , D. Braga , J. Brashear , E. Brondolin , P. Bryant , J. Bueghly , B. Bilki , B. Burkle , A. Butler-Nalin , S. Callier , D. Calvet , X. Cao , B. Caraway , S. Caregari , L. Ceard , Y. C. Cekmecelioglu , G. Cerminara , N. Charitonidis , R. Chatterjee , Y. M. Chen , Z. Chen , K. y. Cheng , S. Chernichenko , H. Cheung , C. H. Chien , S. Choudhury , D. Čoko , G. Collura , F. Couderc , I. Dumanoglu , D. Dannheim , P. Dauncey , A. David , G. Davies , E. Day , P. DeBarbaro , F. De Guio , C. de La Taille , M. De Silva , P. Debbins , E. Delagnes , J. M. Deltoro , G. Derylo , P. G. Dias de Almeida , D. Diaz , P. Dinaucourt , J. Dittmann , M. Dragicevic , S. Dugad , V. Dutta , S. Dutta , J. Eckdahl , T. K. Edberg , M. El Berni , S. C. Eno , Yu. Ershov , P. Everaerts , S. Extier , F. Fahim , C. Fallon , B. A. Fontana Santos Alves , E. Frahm , G. Franzoni , J. Freeman , T. French , E. Gurpinar Guler , Y. Guler , M. Gagnan , P. Gandhi , S. Ganjour , A. Garcia-Bellido , Z. Gecse , Y. Geerebaert , H. Gerwig , O. Gevin , W. Gilbert , A. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , T. Gonzalez , N. Gorbounov , L. Gouskos , Y. Gu , F. Guilloux , E. Gülmez , M. Hammer , A. Harilal , K. Hatakeyama , A. Heering , V. Hegde , U. Heintz , V. Hinger , N. Hinton , J. Hirschauer , J. Hoff , W. S. Hou , C. Isik , J. Incandela , S. Jain , H. R. Jheng , U. Joshi , O. Kara , V. Kachanov , A. Kalinin , R. Kameshwar , A. Kaminskiy , A. Karneyeu , O. Kaya , M. Kaya , A. Khukhunaishvili , S. Kim , K. Koetz , T. Kolberg , A. Kristić , M. Krohn , K. Krüger , N. Kulagin , S. Kulis , S. Kunori , C. M. Kuo , V. Kuryatkov , S. Kyre , O. K. Köseyan , Y. Lai , K. Lamichhane , G. Landsberg , J. Langford , M. Y. Lee , A. Levin , A. Li , B. Li , J. -H. Li , H. Liao , D. Lincoln , L. Linssen , R. Lipton , Y. Liu , A. Lobanov , R. S. Lu , I. Lysova , A. M. Magnan , F. Magniette , A. A. Maier , A. Malakhov , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , P. Masterson , B. Meng , T. Mengke , A. Mestvirishvili , I. Mirza , S. Moccia , I. Morrissey , T. Mudholkar , J. Musić , I. Musienko , S. Nabili , A. Nagar , A. Nikitenko , D. Noonan , M. Noy , K. Nurdan , C. Ochando , B. Odegard , N. Odell , Y. Onel , W. Ortez , J. Ozegović , L. Pacheco Rodriguez , E. Paganis , D. Pagenkopf , V. Palladino , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , J. Parshook , N. Pastika , M. Paulini , P. Paulitsch , T. Peltola , R. Pereira Gomes , H. Perkins , P. Petiot , F. Pitters , F. Pitters , H. Prosper , M. Prvan , I. Puljak , T. Quast , R. Quinn , M. Quinnan , K. Rapacz , L. Raux , G. Reichenbach , M. Reinecke , M. Revering , A. Rodriguez , T. Romanteau , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , A. E. Simsek , U. Sozbilir , O. M. Sahin , A. Sanchez , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , E. Scott , C. Seez , F. Sefkow , S. Sharma , I. Shein , A. Shenai , R. Shukla , E. Sicking , P. Sieberer , Y. Sirois , V. Smirnov , E. Spencer , A. Steen , J. Strait , T. Strebler , N. Strobbe , J. W. Su , E. Sukhov , L. Sun , M. Sun , C. Syal , B. Tali , U. G. Tok , A. Kayis Topaksu , C. L. Tan , I. Tastan , T. Tatli , R. Thaus , S. Tekten , D. Thienpont , T. Pierre-Emile , E. Tiras , M. Titov , D. Tlisov , J. Troska , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , N. Tyurin , S. Undleeb , D. Urbanski , V. Ustinov , A. Uzunian , M. van de Klundert , J. Varela , M. Velasco , M. Vicente Barreto Pinto , P. M. da Silva , T. Virdee , R. Vizinho de Oliveira , J. Voelker , E. Voirin , Z. Wang , X. Wang , F. Wang , M. Wayne , S. N. Webb , M. Weinberg , A. Whitbeck , D. White , R. Wickwire , J. S. Wilson , H. Y. Wu , L. Wu , C. H Yeh , R. Yohay , G. B. Yu , S. S. Yu , D. Yu , F. Yumiceva , A. Zacharopoulou , N. Zamiatin , A. Zarubin , S. Zenz , H. Zhang , J. Zhang

The increased particle flux at the high luminosity phase of the Large Hadron Collider (HL-LHC), with instantaneous luminosities of up to 7.5 times the original design value, will have an impact on many sub-systems of the ATLAS detector.…

Instrumentation and Detectors · Physics 2016-12-22 Thomas G. McCarthy

The use of low-temperature detectors, such as cryogenic calorimeters, has pioneered the recent advancements in low-energy rare event searches. These detectors provide a low-noise environment essential for the direct detection of dark matter…

Instrumentation and Detectors · Physics 2026-02-25 Giorgio Del Castello

In order to fully exploit the physics potential of the Tevatron Run 2, the D0 detector has been upgraded. Having nearly completed the commissioning phase, the D0 detector is starting to produce its first physics results. An overview of the…

High Energy Physics - Experiment · Physics 2007-05-23 Aurelio Juste

The LHC is expected to increase its center-of-mass energy from 13 TeV to 14 TeV for Run 3 scheduled from 2022 to 2024. After Run 3, upgrades for the High-Luminosity-LHC (HL-LHC) programme are planned and the operation will start in 2027,…

Instrumentation and Detectors · Physics 2021-09-01 Yuya Mino

Simulated calorimeter performance in the SiD detector is examined. The software calibration procedures are described, as well as the perfect pattern recognition PFA reconstruction. Performance of the SiD calorimeters is summarized with jet…

Instrumentation and Detectors · Physics 2009-02-17 Ron Cassell

We describe the results of detailed 3-D Monte Carlo simulations of a "CZT calorimeter" that can be used to detect photons in the keV to several MeV range. Several astrophysics applications require the detection of photons in the energy…

Astrophysics · Physics 2009-11-11 I. Jung , H. Krawczynski , S. Komarov , L. Sobotka

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

With the advent of the Tevatron Run 2, the collider experiments, CDF and D0, have reestablished the top quark and the W and Z signals and have begun programs of precision measurements of top quark and electroweak properties. We will survey…

High Energy Physics - Experiment · Physics 2014-11-17 Mark C. Kruse

Many physics topics to be studied by the D0 experiment during Run II of the Fermilab Tevatron ppbar collider give rise to final states containing b--flavored particles. Examples include Higgs searches, top quark production and decay…

The Fermilab Tevatron will be the world's highest energy hadron collider until the LHC is commissioned, it has the world's highest energy fixed target beams, and Fermilab will be the leading high energy physics laboratory in the US for the…

High Energy Physics - Experiment · Physics 2007-05-23 D. Amidei , A. Baden , G. Foster , G. Jackson , T. Kamon , J. Lopez , P. McIntyre , J. Strait , J. White