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The ATLAS Planar Pixel Sensor R&D Project is a collaboration of 17 institutes and more than 80 scientists. Their goal is to explore the operation of planar pixel sensors for the tracker upgrade at the High Luminosity-Large Hadron Collider…

Instrumentation and Detectors · Physics 2015-06-05 Christian Gallrapp

Pixel detectors with cylindrical electrodes that penetrate the silicon substrate (so called 3D detectors) offer advantages over standard planar sensors in terms of radiation hardness, since the electrode distance is decoupled from the bulk…

The upcoming ATLAS Phase II upgrade mandates replacing the tracking system with the all-silicon Inner Tracker (ITK), featuring a pixel detector as its core element. The monitoring data of the new system will be aggregated from an…

Instrumentation and Detectors · Physics 2024-11-04 A. Qamesh , R. Ahmad , M. Karagounis , P. Kind , T. Krawutschke , F. Nitz , L. Schreiter , C. Zeitnitz

3D silicon detectors, in which the electrodes penetrate the sensor bulk perpendicular to the surface, have recently undergone a rapid development from R\&D over industrialisation to their first installation in a real high-energy-physics…

Instrumentation and Detectors · Physics 2015-11-09 Jörn Lange

Pixel sensors based on commercial high-voltage CMOS processes are an exciting technology that is considered as an option for the outer layer of the ATLAS inner tracker upgrade at the High Luminosity LHC. Here, charged particles are detected…

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

Following the Phase-II upgrade during Long Shutdown (LS3), the LHC aims to reach a peak instantaneous luminosity of $7.5\times 10^{34}$cm$^{-2}$s$^{-1}$, which corresponds to an average of around 200 inelastic proton-proton collisions per…

Thin planar pixel modules are promising candidates to instrument the inner layers of the new ATLAS pixel detector for HL-LHC, thanks to the reduced contribution to the material budget and their high charge collection efficiency after…

Instrumentation and Detectors · Physics 2016-09-21 Anna Macchiolo , Richard Nisius , Natascha Savic , Stefano Terzo

The CMS experiment will include a pixel detector for pattern recognition and vertexing. It will consist of three barrel layers and two endcaps on each side, providing three space-points up to a pseudoraditity of 2.1. Taking into account the…

Instrumentation and Detectors · Physics 2009-11-11 R. Horisberger , D. Kotlinski , T. Rohe

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 existing ATLAS Tracker will be at its functional limit for particle fluences of 10^15 neq/cm^2 (LHC). Thus for the upgrades at smaller radii like in the case of the planned Insertable B-Layer (IBL) and for increased LHC luminosities…

The ATLAS detector has to undergo significant updates at the end of the current decade, in order to withstand the increased occupancy and radiation damage that will be produced by the high-luminosity upgrade of the Large Hadron Collider. In…

Instrumentation and Detectors · Physics 2019-08-13 Giovanni Marchiori

The ATLAS experiment pixel detector upgrade plans are focused on development of new technology, including the FE-I4 readout integrated circuit. The first upgrade project to make use of this new technology is an "Insertable B-Layer" (IBL)…

Instrumentation and Detectors · Physics 2011-09-23 M. Garcia-Sciveres , ATLAS Collaboration

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 Phase-1 upgrade of the CMS pixel detector is built out of four barrel layers (BPix) and three forward disks in each endcap (FPix). It comprises a total of 124M pixel channels in 1,856 modules, and it is designed to withstand…

Instrumentation and Detectors · Physics 2017-10-02 Weinan Si

During the shutdown of the CERN Large Hadron Collider in 2013-2014, an additional pixel layer was installed between the existing Pixel detector of the ATLAS experiment and a new, smaller radius beam pipe. The motivation for this new pixel…

Instrumentation and Detectors · Physics 2018-06-07 B. Abbott , J. Albert , F. Alberti , M. Alex , G. Alimonti , S. Alkire , P. Allport , S. Altenheiner , L. Ancu , E. Anderssen , A. Andreani , A. Andreazza , B. Axen , J. Arguin , M. Backhaus , G. Balbi , J. Ballansat , M. Barbero , G. Barbier , A. Bassalat , R. Bates , P. Baudin , M. Battaglia , T. Beau , R. Beccherle , A. Bell , M. Benoit , A. Bermgan , C. Bertsche , D. Bertsche , J. Bilbao de Mendizabal , F. Bindi , M. Bomben , M. Borri , C. Bortolin , N. Bousson , R. Boyd , P. Breugnon , G. Bruni , J. Brossamer , M. Bruschi , P. Buchholz , E. Budun , C. Buttar , F. Cadoux , G. Calderini , L. Caminada , M. Capeans , R. Carney , G. Casse , A. Catinaccio , M. Cavalli-Sforza , M. Červ , A. Cervelli , C. Chau , J. Chauveau , S. Chen , M. Chu , M. Ciapetti , V. Cindro , M. Citterio , A. Clark , M. Cobal , S. Coelli , J. Collot , O. Crespo-Lopez , G. Dalla Betta , C. Daly , G. D'Amen , N. Dann , V. Dao , G. Darbo , C. DaVia , P. David , S. Debieux , P. Delebecque , F. De Lorenzi , R. de Oliveira , K. Dette , W. Dietsche , B. Di Girolamo , N. Dinu , F. Dittus , D. Diyakov , F. Djama , D. Dobos , P. Dondero , K. Doonan , J. Dopke , O. Dorholt , S. Dube , D. Dzahini , K. Egorov , O. Ehrmann , K. Einsweiler , S. Elles , M. Elsing , L. Eraud , A. Ereditato , A. Eyring , D. Falchieri , A. Falou , C. Fausten , A. Favareto , Y. Favre , S. Feigl , S. Fernandez Perez , D. Ferrere , J. Fleury , T. Flick , D. Forshaw , D. Fougeron , L. Franconi , A. Gabrielli , R. Gaglione , C. Gallrapp , K. Gan , M. Garcia-Sciveres , G. Gariano , T. Gastaldi , I. Gavrilenko , A. Gaudiello , N. Geffroy , C. Gemme , F. Gensolen , M. George , P. Ghislain , N. Giangiacomi , S. Gibson , M. Giordani , D. Giugni , H. Gjersdal , K. Glitza , D. Gnani , J. Godlewski , L. Gonella , S. Gonzalez-Sevilla , I. Gorelov , A. Gorišek , C. Gössling , S. Grancagnolo , H. Gray , I. Gregor , P. Grenier , S. Grinstein , A. Gris , V. Gromov , D. Grondin , J. Grosse-Knetter , F. Guescini , E. Guido , P. Gutierrez , G. Hallewell , N. Hartman , S. Hauck , J. Hasi , A. Hasib , F. Hegner , S. Heidbrink , T. Heim , B. Heinemann , T. Hemperek , N. Hessey , M. Hetmánek , R. Hinman , M. Hoeferkamp , T. Holmes , J. Hostachy , S. Hsu , F. Hügging , C. Husi , G. Iacobucci , I. Ibragimov , J. Idarraga , Y. Ikegami , T. Ince , R. Ishmukhametov , J. M. Izen , Z. Janoška , J. Janssen , L. Jansen , L. Jeanty , F. Jensen , J. Jentzsch , S. Jezequel , J. Joseph , H. Kagan , M. Kagan , M. Karagounis , R. Kass , A. Kastanas , C. Kenney , S. Kersten , P. Kind , M. Klein , R. Klingenberg , R. Kluit , M. Kocian , E. Koffeman , O. Korchak , I. Korolkov , I. Kostyukhina-Visoven , S. Kovalenko , M. Kretz , N. Krieger , H. Krüger , A. Kruth , A. Kugel , W. Kuykendall , A. La Rosa , C. Lai , K. Lantzsch , C. Lapoire , D. Laporte , T. Lari , S. Latorre , M. Leyton , B. Lindquist , K. Looper , I. Lopez , A. Lounis , Y. Lu , H. Lubatti , S. Maeland , A. Maier , U. Mallik , F. Manca , B. Mandelli , I. Mandić , D. Marchand , G. Marchiori , M. Marx , N. Massol , P. Mättig , J. Mayer , G. Mc Goldrick , A. Mekkaoui , M. Menouni , J. Menu , C. Meroni , J. Mesa , S. Michal , S. Miglioranzi , M. Mikuž , A. Miucci , K. Mochizuki , M. Monti , J. Moore , P. Morettini , A. Morley , J. Moss , D. Muenstermann , P. Murray , K. Nakamura , C. Nellist , D. Nelson , M. Nessi , R. Nisius , M. Nordberg , F. Nuiry , T. Obermann , W. Ockenfels , H. Oide , M. Oriunno , F. Ould-Saada , C. Padilla , P. Pangaud , S. Parker , G. Pelleriti , H. Pernegger , G. Piacquadio , A. Picazio , D. Pohl , A. Polini , X. Pons , J. Popule , X. Portell Bueso , K. Potamianos , M. Povoli , D. Puldon , Y. Pylypchenko , A. Quadt , B. Quayle , F. Rarbi , F. Ragusa , T. Rambure , E. Richards , C. Riegel , B. Ristic , F. Rivière , F. Rizatdinova , O. Røhne , C. Rossi , L. Rossi , A. Rovani , A. Rozanov , I. Rubinskiy , M. Rudolph , A. Rummler , E. Ruscino , F. Sabatini , D. Salek , A. Salzburger , H. Sandaker , M. Sannino , B. Sanny , T. Scanlon , J. Schipper , U. Schmidt , B. Schneider , A. Schorlemmer , N. Schroer , P. Schwemling , A. Sciuccati , S. Seidel , A. Seiden , P. Šícho , P. Skubic , M. Sloboda , D. Smith , M. Smith , A. Sood , E. Spencer , M. Stramaglia , M. Strauss , S. Stucci , B. Stugu , J. Stupak , N. Styles , D. Su , Y. Takubo , J. Tassan , P. Teng , A. Teixeira , S. Terzo , X. Therry , T. Todorov , M. Tomášek , K. Toms , R. Travaglini , W. Trischuk , C. Troncon , G. Troska , S. Tsiskaridze , I. Tsurin , D. Tsybychev , Y. Unno , L. Vacavant , B. Verlaat , E. Vigeolas , M. Vogt , V. Vrba , R. Vuillermet , W. Wagner , W. Walkowiak , R. Wang , S. Watts , M. Weber , M. Weber , J. Weingarten , S. Welch , S. Wenig , M. Wensing , N. Wermes , T. Wittig , M. Wittgen , T. Yildizkaya , Y. Yang , W. Yao , Y. Yi , A. Zaman , R. Zaidan , C. Zeitnitz , M. Ziolkowski , V. Zivkovic , A. Zoccoli , L. Zwalinski

The High Luminosity LHC (HL-LHC) upgrade requires the planned Inner Tracker (ITk) of the ATLAS detector to tolerate extremely high radiation doses. Specifically, the innermost parts of the pixel system will have to withstand radiation…

We report on preliminary design studies of a pixel detector for CMS at the Super-LHC. The goal of these studies was to investigate the possibility of designing an inner tracker pixel detector whose data could be used for selecting events at…

Instrumentation and Detectors · Physics 2007-05-23 J. Jones , G. Hall , C. Foudas , A. Rose

In the framework of the HL-LHC upgrade, the ATLAS experiment plans to introduce an all-silicon inner tracker to cope with the elevated occupancy. To investigate the suitability of pixel sensors using the proven planar technology for the…

Instrumentation and Detectors · Physics 2015-06-23 C. Nellist

To cope with the High Luminosity LHC harsh conditions, the ATLAS inner tracker has to be upgraded to meet requirements in terms of radiation hardness, pile up and geometrical acceptance. The active edge technology allows to reduce the…