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Related papers: The Alignment of the ATLAS Silicon Tracker

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The Robust Alignment algorithm for the ATLAS silicon detectors is presented. It is an iterative method based on centering residual and overlap residual distributions. Tests on simulated and real data are discussed.

Instrumentation and Detectors · Physics 2007-10-08 Florian Heinemann

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 central component of the CMS detector is the largest silicon tracker ever built. The precise alignment of this complex device is a formidable challenge, and only achievable with a significant extension of the technologies routinely used…

Instrumentation and Detectors · Physics 2014-08-22 CMS Collaboration

The complex system of the CMS all-silicon Tracker, with 15\,148 silicon strip and 1440 silicon pixel modules, requires sophisticated alignment procedures. In order to achieve an optimal track-parameter resolution, the position and…

Instrumentation and Detectors · Physics 2011-08-31 Claus Kleinwort , Frank Meier

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

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

This conference proceeding presents the first results of the full CMS Tracker alignment based on several million reconstructed tracks from the cosmic data taken during the commissioning runs with the detector in its final position and…

Instrumentation and Detectors · Physics 2011-05-18 Frank Meier

The CMS silicon tracker, consisting of 1440 silicon pixel and 15148 silicon strip detector modules, has been aligned using more than three million cosmic ray charged particles, with additional information from optical surveys. The positions…

Instrumentation and Detectors · Physics 2012-08-27 CMS Collaboration

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

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

Track detectors in high energy physics experiments require an accurate determination of a large number of alignment parameters. A general method has been developed, which allows the determination of up to several thousand alignment…

High Energy Physics - Experiment · Physics 2007-05-23 Volker Blobel , Claus Kleinwort

This report presents recent results on track reconstruction and alignment with the silicon tracker of the CMS experiment at the LHC, obtained with a full detector simulation. After an overview of the layout of the tracker and its material…

Instrumentation and Detectors · Physics 2007-05-23 F. -P. Schilling

The ATLAS Inner Detector is a composite tracking system consisting of silicon pixels, silicon strips and straw tubes in a 2 T magnetic field. Its installation was completed in August 2008 and the detector took part in data- taking with…

Instrumentation and Detectors · Physics 2012-08-27 The ATLAS Collaboration

The inner silicon detector of the Compact Muon Solenoid experiment (CMS) at CERN's LHC consists of 16588 modules. Charged-particle tracks in the detector are used to improve the accuracy to which the position and orientation of the modules…

Instrumentation and Detectors · Physics 2015-05-27 Volker Blobel , Claus Kleinwort , Frank Meier

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 inner tracking system of the CMS experiment, which comprises Silicon Pixel and Silicon Strip detectors, is designed to provide a precise measurement of the momentum of charged particles and to reconstruct the primary and secondary…

High Energy Physics - Experiment · Physics 2023-02-08 Sandra Consuegra Rodríguez

The alignment of the ATLAS Inner Detector is performed with a track-based algorithm. The aim of the detector alignment is to provide an accurate description of the detector geometry such that track parameters are accurately determined and…

Instrumentation and Detectors · Physics 2019-10-15 Julian Wollrath

The strategies for and the performance of the CMS silicon tracking system alignment during the 2015-2018 data-taking period of the LHC are described. The alignment procedures during and after data taking are explained. Alignment scenarios…

Instrumentation and Detectors · Physics 2022-06-15 CMS Collaboration

The ATLAS Semiconductor Tracker (SCT) together with the pixel and the transition radiation detectors will form the tracking system of the ATLAS experiment at LHC. It will consist of 20000 single-sided silicon microstrip sensors assembled…

Instrumentation and Detectors · Physics 2019-08-14 Vasiliki A. Mitsou

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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