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Related papers: Recent Progress on 3D Silicon Detectors

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CMOS Pixel Sensors are making steady progress towards the specifications of the ILD vertex detector. Recent developments are summarised, which show that these devices are close to comply with all major requirements, in particular the…

Accurate 3D imaging is essential for machines to map and interact with the physical world. While numerous 3D imaging technologies exist, each addressing niche applications with varying degrees of success, none have achieved the breadth of…

The Compact Linear Collider (CLIC) is a high-energy high-luminosity linear electron-positron collider under development. It is foreseen to be built and operated in three stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV,…

Instrumentation and Detectors · Physics 2019-05-08 A. C. Abusleme Hoffman , G. Parès , T. Fritzsch , M. Rothermund , H. Jansen , K. Krüger , F. Sefkow , A. Velyka , J. Schwandt , I. Perić , L. Emberger , C. Graf , A. Macchiolo , F. Simon , M. Szalay , N. van der Kolk , H. Abramowicz , Y. Benhammou , O. Borysov , M. Borysova , A. Joffe , S. Kananov , A. Levy , I. Levy , G. Eigen , R. Bugiel , S. Bugiel , M. Firlej , T. A. Fiutowski , M. Idzik , J. Moroń , K. P. Świentek , P. Terlecki , P. Brückman de Renstrom , B. Turbiarz , T. Wojtoń , L. K. Zawiejski , E. Firu , V. Ghenescu , A. T. Neagu , T. Preda , I. Boyko , Yu. Nefedov , A. Rymbekova , A. Sapronov , G. Shelkov , A. Zhemchugov , A. Ruiz-Jimeno , I. Vila , E. Fullana , J. Fuster , P. Gomis Lopez , M. Perelló , M. A. Villarejo , M. Vos , J. Alozy , N. Alipour Tehrani , D. Arominski , R. Ballabriga Sune , F. Boyer , E. Brondolin , M. Buckland , M. Campbell , D. Dannheim , K. Dette , F. Duarte Ramos , N. Egidos Plaja , K. Elsener , A. Fiergolski , C. Fuentes Rojas , C. Grefe , D. Hynds , W. Klempt , I. Kremastiotis , J. Kröger , S. Kulis , E. Leogrande , L. Linssen , X. Llopart Cudie , A. Lucaci-Timoce , M. Munker , L. Musa , A. Nürnberg , F. -X. Nuiry , E. Perez Codina , H. Pernegger , M. Petrič , F. Pitters , T. Quast , S. Redford , P. Riedler , P. Roloff , A. Sailer , E. Santin , U. Schnoor , E. Sicking , K. Sielewicz , R. Simoniello , W. Snoeys , S. Spannagel , S. Sroka , R. Ström , P. Valerio , S. van Dam , E. van der Kraaij , T. Vǎnát , O. Viazlo , M. Vicente Barreto Pinto , M. A. Weber , M. Williams , K. Wolters , M. Benoit , G. Iacobucci , D M S Sultan , R. R. Bosley , T. Price , M. F. Watson , N. K. Watson , A. G. Winter , J. Goldstein , S. Green , J. S. Marshall , M. A. Thomson , B. Xu , G. Casse , J. Vossebeld , T. Coates , F. Salvatore , J. Repond , L. Xia , C. Kenney , A. Tomada

This report reviews current trends in the R&D of semiconductor pixellated sensors for vertex tracking and radiation imaging. It identifies requirements of future HEP experiments at colliders, needed technological breakthroughs and…

In view of the High Luminosity upgrade of the Large Hadron Collider (HL-LHC), planned to start around 2023-2025, the ATLAS experiment will undergo a replacement of the Inner Detector. A higher luminosity will imply higher irradiation levels…

Instrumentation and Detectors · Physics 2016-12-21 N. Savic , J. Beyer , A. La Rosa , A. Macchiolo , R. Nisius

For the Phase-II Upgrade of the ATLAS detector at CERN, the current ATLAS Inner Detector will be replaced with the ATLAS Inner Tracker. The ATLAS Inner Tracker will be an all-silicon detector, consisting of a pixel tracker and a strip…

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…

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

For the ATLAS Pixel Detector fast readout electronics has been successfully developed and tested. Main attention was given to the ability to detect small charges in the order of 5,000 electrons within 25 ns in the harsh radiation…

Instrumentation and Detectors · Physics 2008-11-26 Fabian Huegging

We report on the development of 3D silicon sensors at the University of Science and Technology of China (USTC). The sensor involves columnar electrodes (5 um in diameter) of both doping types, etched from the same wafer side. The p+…

Instrumentation and Detectors · Physics 2026-05-14 Kuo Ma , De Zhang , Shengjia He , Tian-ao Wang , Han Li , Yu Nie , Xiuxia Wang , Jinlan Peng , Zheng Liang , Xiang Li , Wenhua Shi , Manwen Liu , Chuan Liao , Zheng Li , Zebo Tang , Yanwen Liu

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 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

Detectors based on pixels with timing capabilities are gaining increasing importance in the last years. Next-to-come high-energy physics experiments at colliders requires the use of time information in tracking, due to the increasing levels…

Instrumentation and Detectors · Physics 2020-08-25 Adriano Lai , Gian Matteo Cossu

The challenging demands of the ATLAS High Luminosity (HL-LHC) Upgrade aim for a complete swap of new generation sensors that should cope with the ultimate radiation hardness. FBK has been one of the prime foundries to develop and fabricate…

Instrumentation and Detectors · Physics 2022-09-29 D M S Sultan , Md Arif Abdulla Samy , J. X. Ye , M. Boscardin , F. Ficorella , S. Ronchin , G. -F. Dalla Betta

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. Because of its radiation hardness and cost effectiveness, the n-on-p silicon…

Instrumentation and Detectors · Physics 2013-11-18 M. Bomben , A. Bagolini , M. Boscardin , L. Bosisio , G. Calderini , J. Chauveau , G. Giacomini , A. La Rosa , G. Marchori , N. Zorzi

There exists an enormous interest for the study of very high energy domain in particle physics, both theoretically and experimentally, in the aim to construct a general theory of the fundamental constituents of matter and of their…

Instrumentation and Detectors · Physics 2007-05-23 I. Lazanu , S. Lazanu

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

During the LHC Long Shutdown 3 (2026-29) ALICE will replace its three innermost tracking layers by a new detector, the "ITS3". It will be based on newly developed, wafer-scale monolithic active pixel sensors, which are bent into truly…

Instrumentation and Detectors · Physics 2026-01-13 Jory Sonneveld

The ATLAS collaboration will replace its tracking detector with new all silicon pixel and strip systems. This will allow to cope with the higher radiation and occupancy levels expected after the 5-fold increase in the luminosity of the LHC…

Pixel vertex detectors are THE instrument of choice for the tracking of charged particles close to the interaction point at the LHC. Hybrid pixel detectors, in which sensor and read-out IC are separate entities, constitute the present state…

Instrumentation and Detectors · Physics 2009-09-29 Norbert Wermes