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The future ATLAS ITk strip tracker will consist of 17,000 silicon strip detector modules mounted on support structures called cores. Cores are assembled from a number of components, among others carbon fibre facings, honeycomb structure and…

Instrumentation and Detectors · Physics 2021-03-11 Luise Poley , Tim Jones

The ATLAS experiment will undergo a major upgrade of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) foreseen to start around 2025. Thin planar pixel modules are promising candidates to instrument the new pixel…

Instrumentation and Detectors · Physics 2017-03-08 N. Savic , L. Bergbreiter , J. Breuer , A. La Rosa , A. Macchiolo , R. Nisius , S. Terzo

The ATLAS experiment at the LHC will replace its current inner tracker system for the HL-LHC era. 3D silicon pixel sensors are being considered as radiation-hard candidates for the innermost layers of the new fully silicon-based tracking…

Instrumentation and Detectors · Physics 2019-09-04 S. Terzo , M. Chmeissani , G. Giannini , S. Grinstein , M. Manna , G. Pellegrini , D. Quirion , D. Vazquez Furelos

While the tracking detectors of the ATLAS and CMS experiments have shown excellent performance in Run 1 of LHC data taking, and are expected to continue to do so during LHC operation at design luminosity, both experiments will have to…

The LHCb experiment is preparing for a major upgrade in 2018-2019. One of the key components in the upgrade is a new silicon tracker situated upstream of the analysis magnet of the experiment. The Upstream Tracker (UT) will consist of four…

The Silicon Strip Detector (SSD) is a fundamental part of the Inner Tracking System (ITS) for the ALICE experiment. Since the early phase of proton-proton collisions at LHC, the SSD is fully operational and participating in the charged…

Instrumentation and Detectors · Physics 2019-08-13 Giacomo Contin

The ATLAS Forward Proton (AFP) detector is designed to identify events in which one or two protons emerge intact from the LHC collisions. AFP will consist of a tracking detector, to measure the momentum of the protons, and a time of flight…

The next generation Advanced ACTPol (AdvACT) experiment is currently underway and will consist of four Transition Edge Sensor (TES) bolometer arrays, with three operating together, totaling ~5800 detectors on the sky. Building on experience…

Test beam studies of ITk pixel sensors and full modules are an essential tool for assessing their performance and operational behavior. In the 2025 test beam campaigns, quad and triplet modules equipped with both pre-production and…

The ATLAS experiment will undergo a major upgrade of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) to start operation in 2026. The most severe challenges are to be faced by the innermost layers of the pixel…

Instrumentation and Detectors · Physics 2016-12-06 Julien-Christopher Beyer , Alessandro La Rosa , Anna Macchiolo , Richard Nisius , Natascha Savic

The Inner Tracking System (ITS) is the key ALICE detector for the study of heavy flavour production at LHC. Heavy flavor can be studied via the identification of short-lived hadrons containing heavy quarks which have a mean proper decay…

Instrumentation and Detectors · Physics 2015-06-12 Stefan Rossegger

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 Insertable B-Layer (IBL) is the innermost layer of pixel detectors, and was installed in May 2014 at a radius of 3.3 cm from the beam axis, between the existing Pixel detector and a new smaller radius beam-pipe. The new detector,…

Instrumentation and Detectors · Physics 2017-01-16 Alessandro La Rosa

The CMS Inner Tracker, made of silicon pixel modules, will be entirely replaced prior to the start of the High Luminosity LHC period. One of the crucial components of the new Inner Tracker system is the readout chip, being developed by the…

Instrumentation and Detectors · Physics 2021-11-01 Natalia Emriskova

The front-end electronics of silicon detectors are typically designed to ensure optimal noise performance for the expected input charge. A combination of preamplifiers and shaper circuits result in a nontrivial response of the front-end to…

Instrumentation and Detectors · Physics 2024-07-02 M. J. Basso , E. Buchanan , B. J. Gallop , J. J. John , J. Kaplon , P. T. Keener , P. W. Phillips , L. Poley , C. A. Sawyer , D. Sperlich , M. Warren

To extend the physics reach of the LHC, accelerator upgrades are planned which will increase the integrated luminosity to beyond 3000 fb^-1 and the pile-up per bunch-crossing by a factor 5 to 10. To cope with the increased occupancy and…

Instrumentation and Detectors · Physics 2015-06-17 G. Calderini

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 ATLAS experiment is planning a complete replacement of its inner detector(ID) with a new all-silicon inner tracker (ITk) for the ATLAS Inner Tracker Phase-2 upgrade. The ATLAS18 silicon strip sensors are designed to operate up to the…

Instrumentation and Detectors · Physics 2025-03-26 Y. Huang , H. Li , B. Crick , V. Cindro , A. Chisholm , M. Cai , H. Deng , V. Fadeyev , S. Hirose , H. Jing , B. Jiang , P. Liu , Y. Liu , W. Lu , H. Liu , I. Mandić , R. S. Orr , X. Shi , Z. Tan , Y. Unno , M. Ullan , S. Wang , Z. Xu

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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