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ATLAS is a multipurpose experiment at the LHC. The tracking system of ATLAS, embedded in a 2 T solenoidal field, is composed of different technologies: silicon planar sensors (pixel and microstrips) and drift-tubes. The procedure used to…

Instrumentation and Detectors · Physics 2019-08-13 Ana Ovcharova

The ATLAS Inner Detector is responsible for particle tracking in ATLAS experiment at CERN Large Hadron Collider (LHC) and comprises silicon and gas based detectors. The combination of both silicon and gas based detectors provides high…

Instrumentation and Detectors · Physics 2019-08-13 Ewa Stanecka

The ATLAS detector, built at one of the interaction points of the Large Hadron Collider, is operational and has been collecting data from cosmic rays. This paper describes the track based alignment of the ATLAS Inner Detector tracker which…

Instrumentation and Detectors · Physics 2019-08-13 Grant Gorfine

The ATLAS detector at CERN's Large Hadron Collider (LHC) is equipped with a tracking system at its core (the Inner Detector, ID) consisting of silicon and gaseous straw tube detectors. The physics performance of the ID requires a precision…

Instrumentation and Detectors · Physics 2019-08-13 Muge Karagoz Unel

The ATLAS pixel detector is the innermost detector of the ATLAS experiment at the Large Hadron Collider at CERN. With approximately 80 million readout channels, the ATLAS silicon pixel detector is a high-acceptance, high-resolution,…

Instrumentation and Detectors · Physics 2019-08-13 E. Galyaev

The ATLAS Pixel detector is a high-resolution, low-noise silicon-based device designed to provide tracking and vertexing information within a distance of 12 cm from the LHC beam axis. It consists of approximately 80 million pixel channels…

Instrumentation and Detectors · Physics 2019-08-13 J. Biesiada

The performance of the ATLAS Inner Detector alignment has been studied using $pp$ collision data at $\sqrt{s} = 13$ TeV collected by the ATLAS experiment during Run 2 (2015 to 2018) of the Large Hadron Collider (LHC). The goal of the…

High Energy Physics - Experiment · Physics 2021-01-05 ATLAS Collaboration

The ATLAS inner detector comprises three different sub-detectors: the pixel detector, the silicon strip tracker, and the transition-radiation drift-tube tracker. The Insertable $B$-Layer, a new innermost pixel layer, was installed during…

High Energy Physics - Experiment · Physics 2017-12-08 ATLAS Collaboration

The Semiconductor Tracker (SCT) is a silicon strip detector and one of the key precision tracking devices in the Inner Detector of the ATLAS experiment at CERN LHC. The completed SCT has been installed inside the ATLAS experimental cavern…

Instrumentation and Detectors · Physics 2019-08-13 Vasiliki A. Mitsou

ALICE (A Large Ion Collider Experiment) is the LHC (Large Hadron Collider) experiment devoted to investigating the strongly interacting matter created in nucleus-nucleus collisions at the LHC energies. The ALICE ITS, Inner Tracking System,…

Instrumentation and Detectors · Physics 2017-10-02 ALICE Collaboration

The semiconductor tracker is a silicon microstrip detector forming part of the inner tracking system of the ATLAS experiment at the LHC. The operation and performance of the semiconductor tracker during the first years of LHC running are…

High Energy Physics - Experiment · Physics 2015-06-19 ATLAS Collaboration

ATLAS is one of the two general purpose detectors at the world's largest particle accelerator, the Large Hadron Collider (LHC). The LHC will be colliding proton beams at a center of mass energy {\surd}s= 14 TeV and is currently operating at…

Instrumentation and Detectors · Physics 2010-10-11 Mahsana Ahsan

The ATLAS Inner Tracker, the future innermost part of the ATLAS detector, is an all-silicon tracker composed of pixel and strip modules, designed to cope with the extreme conditions expected during High-Luminosity LHC runs. Thorough testing…

We discuss the track-based alignment for the Inner Detector of the ATLAS experiment. After describing the main alignment method based on the minimization of hit residuals, we focus on alignment methods using information from the…

High Energy Physics - Experiment · Physics 2019-08-13 Jochen Schieck

The ATLAS inner detector is used to reconstruct secondary vertices due to hadronic interactions of primary collision products, so probing the location and amount of material in the inner region of ATLAS. Data collected in 7 TeV pp…

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

The ALICE detector was designed to track and identify particles in a wide transverse momentum range, from more than 100 GeV/c down to ~100 MeV/c. The innermost barrel-like detector, the Inner Tracking System (ITS), is dedicated to precise…

Instrumentation and Detectors · Physics 2019-08-13 Andrea Rossi

The Inner Tracking System (ITS) Upgrade for the ALICE experiment at LHC is the first large-area ($\sim$10~m$^2$) silicon vertex detector based on the CMOS Monolithic Active Pixel Sensor (MAPS) technology, which combines sensitive volume and…

Instrumentation and Detectors · Physics 2020-01-10 G. Contin

The new Inner Tracking System (ITS2) is instrumental for tracking and vertex reconstruction in the ALICE experiment. The new tracker consists of seven cylindrical layers equipped with silicon Monolithic Active Pixel Sensors (MAPS) with a…

Instrumentation and Detectors · Physics 2025-05-21 A. Isakov

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

A small set of final prototypes of the ATLAS Inner Detector silicon tracker (Pixel and SCT) were used to take data during the 2004 Combined Test Beam. Data were collected from runs with beams of different flavour (electrons, pions, muons…

Instrumentation and Detectors · Physics 2010-05-12 A. Ahmad , A. Andreazza , T. Atkinson , J. Baines , A. J. Barr , R. Beccherle , P. J. Bell , J. Bernabeu , Z. Broklova , P. A. Bruckman de Renstrom , D. Cauz , L. Chevalier , S. Chouridou , M. Citterio , A. Clark , M. Cobal , T. Cornelissen , S. Correard , M. J. Costa , D. Costanzo , S. Cuneo , M. Dameri , G. Darbo , J. B. de Vivie , B. Di Girolamo , D. Dobos , Z. Drasal , J. Drohan , K. Einsweiler , M. Elsing , D. Emelyanov , C. Escobar , K. Facius , P. Ferrari , D. Fergusson , D. Ferrere , T. Flick , D. Froidevaux , G. Gagliardi , M. Gallas , B. J. Gallop , K. K. Gan , C. Garcia , I. L. Gavrilenko , C. Gemme , P. Gerlach , T. Golling , S. Gonzalez-Sevilla , M. J. Goodrick , G. Gorfine , T. Goettfert , J. Grosse-Knetter , P. H. Hansen , K. Hara , R. Hartel , A. Harvey , R. J. Hawkings , F. E. W. Heinemann , T. Henns , J. C. Hill , F. Huegging , E. Jansen , J. Joseph , M. Karagoz Unel , M. Kataoka , S. Kersten , A. Khomich , R. Klingenberg , P. Kodys , T. Koffas , N. Konstantinidis , V. Kostyukhin , C. Lacasta , T. Lari , S. Latorre , C. G. Lester , W. Liebig , A. Lipniacka , K. F. Lourerio , M. Mangin-Brinet , S. Marti i Garcia , M. Mathes , C. Meroni , B. Mikulec , B. Mindur , S. Moed , G. Moorhead , P. Morettini , E. W. J. Moyse , K. Nakamura , P. Nechaeva , K. Nikolaev , F. Parodi , S. Parzhitski , J. Pater , R. Petti , P. W. Phillips , B. Pinto , A. Poppleton , K. Reeves , I. Reisinger , P. Reznicek , P. Risso , D. Robinson , S. Roe , A. Rozanov , A. Salzburger , H. Sandaker , L. Santi , C. Schiavi , J. Schieck , J. Schultes , A. Sfyrla , C. Shaw , F. Tegenfeldt , C. J. W. P. Timmermans , B. Toczek , C. Troncon , M. Tyndel , F. Vernocchi , J. Virzi , T. Vu Anh , M. Warren , J. Weber , M. Weber , A. R. Weidberg , J. Weingarten , P. S. Wells , A. Zhelezko
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