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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

In view of the LHC upgrade phases towards the High Luminosity LHC (HL-LHC), the ATLAS experiment plans to upgrade the Inner Detector with an all-silicon system. The n-on-p silicon technology is a promising candidate to achieve a large area…

The ATLAS pixel detector is a high precision silicon tracking device located closest to the LHC interaction point. It belongs to the first generation of its kind in a hadron collider experiment. It will provide crucial pattern recognition…

Instrumentation and Detectors · Physics 2019-08-13 J. -F. Arguin

The high-luminosity upgrade of the CERN LHC requires the replacement of the CMS tracking detector to cope with the increased radiation fluence while maintaining its excellent performance. An extensive R\&D program, aiming at using 3D pixel…

Instrumentation and Detectors · Physics 2025-10-16 The Tracker Group of the CMS Collaboration

The innermost part of the tracking detector of the ATLAS experiment consists mainly of planar n$^+$-in-n silicon pixel sensors. During the phase-0 upgrade, the Insertable B-Layer (IBL) was installed closest to the beam pipe. Its pixels are…

Instrumentation and Detectors · Physics 2018-08-21 A. Gisen , S. Altenheiner , C. Gößling , M. Grothe , R. Klingenberg , K. Kröninger , J. Lönker , M. Weers , T. Wittig , F. Wizemann

The upgrade to the High Luminosity Large Hadron Collider will pose unprecedented challenges to the tracking systems of all experiments. Recent advancement of active pixel detectors designed in CMOS processes provide attractive alternatives…

Instrumentation and Detectors · Physics 2017-09-13 T. Bisanz , J. Große-Knetter , A. Quadt , J. Rieger , J. Weingarten

The upgrade of the Inner Tracking System (ITS) of ALICE is planned for the second long shutdown of the LHC in 2019-2020. The ALICE physics program after the shutdown requires the ITS to have improved tracking capabilities and improved…

Instrumentation and Detectors · Physics 2015-11-30 Monika Kofarago

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 Inner Tracking System (ITS) of the ALICE experiment will be upgraded during the second long LHC shutdown in $\mathrm{2019}-\mathrm{2020}$. The main goal of the ALICE ITS Upgrade is to enable high precision measurements of low - momentum…

Instrumentation and Detectors · Physics 2019-05-22 D. Andreou

The ALICE Experiment at the Large Hadron Collider (LHC) underwent a major upgrade during the Long Shutdown 2. Several subsystems have been improved, including the ALICE Inner Tracking System (ITS), which has been entirely replaced. The new…

Instrumentation and Detectors · Physics 2024-10-01 Andrea Sofia Triolo

In view of the LHC upgrade for the High Luminosity Phase (HL-LHC), the ATLAS experiment is planning to replace the Inner Detector with an all-Silicon system. The n-in-p bulk technology represents a valid solution for the modules of most of…

Instrumentation and Detectors · Physics 2015-06-17 G. Calderini , A. Bagolini , M. Bomben , M. Boscardin , L. Bosisio , J. Chauveau , G. Giacomini , A. La Rosa , G. Marchiori , N. Zorzi

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…

Pixel detectors are used in the innermost part of multi purpose experiments at the Large Hadron Collider (LHC) and are therefore exposed to the highest fluences of ionising radiation, which in this part of the detectors consists mainly of…

Instrumentation and Detectors · Physics 2010-01-21 T. Rohe , J. Acosta , A. Bean , S. Dambach , W. Erdmann , U. Langenegger , C. Martin , B. Meier , V. Radicci , J. Sibille , P. Trueb

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

Construction of the new all-silicon Inner Tracker (ITk), developed by the ATLAS collaboration for the High Luminosity LHC, started in 2020 and is expected to continue till 2028. The ITk detector will include 18,000 highly segmented and…

The ATLAS detector is currently being upgraded with a new layer of pixel based charged particle tracking and a new arrangement of the services for the pixel detector. These upgrades require the replacement of the opto-boards previously used…

Instrumentation and Detectors · Physics 2013-10-04 Richard Kass , K. K. Gan , H. P. Kagan , J. Moss , J. Moore , S. Smith , Y. Yang , P. Buchholz , M. Ziolkowski

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

In view of the LHC upgrade phases towards HL-LHC the ATLAS experiment plans to upgrade the Inner Detector with an all silicon system. The n-in-p silicon technology is a promising candidate for the pixel upgrade thanks to its radiation…

Instrumentation and Detectors · Physics 2015-06-05 A. La Rosa , C. Gallrapp , A. Macchiolo , R. Nisius , H. Pernegger , R. H. Richter , P. Weigell

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 upgrade of the Inner Tracking System (ITS) of ALICE (A Large Ion Collider Experiment) will extend measurements of heavy-flavour hadrons and low-mass dileptons to a lower transverse momentum than currently achieved and increase the…

Instrumentation and Detectors · Physics 2020-08-26 James Philip Iddon
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