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The ALICE Inner Tracking System has been recently upgraded to a full silicon detector consisting entirely of MAPS, arranged in seven concentric layers around the LHC beam pipe. Further ahead, during the LHC Long Shutdown 3, the ALICE…

Instrumentation and Detectors · Physics 2022-09-21 Bogdan-Mihail Blidaru

ALICE, one of the four main CERN LHC experiments, studies heavy-ion collisions at ultra-relativistic energies. For LHC Run 4 (starting 2030), ALICE will replace the three innermost cylindrical layers of its inner tracking system during Long…

Instrumentation and Detectors · Physics 2025-05-07 Livia Terlizzi

CMOS pixel sensors (CPS) represent a novel technological approach to building charged particle detectors. CMOS processes allow to integrate a sensing volume and readout electronics in a single silicon die allowing to build sensors with a…

Monolithic Active Pixel Sensors (MAPS) combine the sensing part and the front-end electronics in the same silicon layer, making use of CMOS technology. Profiting from the progresses of this commercial process, MAPS have been undergoing…

Instrumentation and Detectors · Physics 2024-08-06 Domenico Colella

The Inner Tracking System (ITS) Upgrade for the ALICE experiment at LHC is the first large-area ($\sim$10~m$^2$) silicon vertex detector based on the CMOS Monolithic Active Pixel Sensor (MAPS) technology, which combines sensitive volume and…

Instrumentation and Detectors · Physics 2020-01-10 G. Contin

The new Inner Tracking System (ITS2) is instrumental for tracking and vertex reconstruction in the ALICE experiment. The new tracker consists of seven cylindrical layers equipped with silicon Monolithic Active Pixel Sensors (MAPS) with a…

Instrumentation and Detectors · Physics 2025-05-21 A. Isakov

Monolithic active pixel sensors (MAPS) produced in a 65 nm CMOS imaging technology are being investigated for applications in particle physics. The MAPS design has a small collection electrode characterized by an input capacitance of ~fF,…

Active Pixel Sensor (APS) technology has shown promise for next-generation vertex detectors. This paper discusses the design and testing of two generations of APS chips. Both are arrays of 128 by 128 pixels, each 20 by 20 micro-m. Each…

Nuclear Experiment · Physics 2011-07-19 H. S. Matis , F. Bieser , S. Kleinfelder , G. Rai , F. Retiere , H. G. Ritter , K. Singh , S. E. Wurzel , H. Wieman , E. Yamamoto

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

The silicon pixel detector (SPD) of the ALICE experiment in preparation at the Large Hadron Collider (LHC) at CERN is designed to provide the precise vertex reconstruction needed for measuring heavy flavor production in heavy ion collisions…

Nuclear Experiment · Physics 2012-07-07 Jan Conrad

During Large Hadron Collider (LHC) Long Shutdown 3 (LS3) (2026-28), the ALICE experiment is replacing its inner-most three tracking layers by a new detector, Inner Tracking System 3. It will be based on newly developed wafer-scale…

Instrumentation and Detectors · Physics 2024-09-04 Chun-Zheng Wang

CMOS Monolithic Active Pixel Sensors (CPS) are ultra-light and highly granular silicon pixel detectors suited for highly sensitive charged particle tracking. Being manufactured with cost efficient standard CMOS processes, CPS may integrate…

Instrumentation and Detectors · Physics 2020-01-29 M. Deveaux

The performance of novel n-in-p planar pixel detectors, designed for future upgrades of the ATLAS Pixel system is presented. The n-in-p silicon sensors technology is a promising candidate for the pixel upgrade thanks to its radiation…

Instrumentation and Detectors · Physics 2012-04-13 C. Gallrapp , A. La Rosa , A. Macchiolo , R. Nisius , H. Pernegger , R. H. Richter , P. Weigell

For the Inner Tracking System 3 (ITS3) upgrade, the ALICE experiment at CERN requires monolithic active pixel sensors of dimensions up to 97~mm$\,\times\,$266~mm, occupying a large fraction of a 300 mm wafer. To manufacture such a…

CMOS sensors were successfully implemented in the STAR tracker [1]. LHC experiments have shown that efficient b tagging, reconstruction of displaced vertices and identification of disappearing tracks are necessary. An improved vertex…

Instrumentation and Detectors · Physics 2021-05-21 Nicolas T. Fourches , Geraldine Hallais , Charles Renard

The high integration density of MAPS, with silicon sensor and readout electronics implemented in the same device, allows very thin structures with a greatly reduced material budget. Thicknesses of $\mathcal{O}$(50~$\mu$m), values at which…

Instrumentation and Detectors · Physics 2022-10-05 Domenico Colella

The ALICE Inner Tracking System upgrade (ITS3) will employ stitched, wafer-scale Monolithic Active Pixel Sensors (MAPS) for the first time in high-energy physics, achieving a material budget of only 0.09$\,$%$\,$X$\mathrm{_{0}}$ per layer.…

Instrumentation and Detectors · Physics 2025-11-05 Marius Wilm Menzel

During the second LHC long shutdown (LS2) the Inner Tracking System (ITS) of ALICE (A Large Ion Collider Experiment) will be replaced by seven layers of CMOS Monolithic Active Pixel Sensors (MAPS). The latest innovations in silicon imaging…

Nuclear Experiment · Physics 2020-05-01 D. Andreou

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 new Inner Tracking System (ITS2) of the ALICE experiment began operation in 2021 with the start of LHC Run 3. Compared to its predecessor, ITS2 offers substantial improvements in pointing resolution, tracking efficiency at low…

Instrumentation and Detectors · Physics 2026-04-15 D. Agguiaro , G. Aglieri Rinella , L. Aglietta , M. Agnello , F. Agnese , B. Alessandro , G. Alfarone , J. Alme , E. Anderssen , D. Andreou , M. Angeletti , N. Apadula , P. Atkinson , C. Azzan , R. Baccomi , A. Badalà , A. Balbino , P. Barberis , F. Barile , L. Barioglio , R. Barthel , F. Baruffaldi , N. K. Behera , I. Belikov , A. Benato , M. Benettoni , F. Benotto , S. Beole , N. Bez , A. Bhatti , M. Bhopal , A. P. Bigot , G. Boca , G. Bonomi , M. Bonora , F. Borotto Dalla Vecchia , M. Borri , V. Borshchov , E. Botta , L. Boynton , G. Brower , E. Bruna , O. Brunasso Cattarello , G. E. Bruno , M. D. Buckland , S. Bufalino , P. Camerini , P. Cariola , C. Ceballos Sanchez , J. Cho , S. Cho , K. Choi , Y. Choi , N. J. Clague , O. A. Clausse , F. Colamaria , D. Colella , S. Coli , A. Collu , M. Concas , G. Contin , Y. Corrales Morales , S. Costanza , J. B. Dainton , E. Danè , W. Degraw , C. De Martin , W. Deng , G. De Robertis , P. Dhankher , A. Di Mauro , F. Dumitrache , D. Elia , M. R. Ersdal , J. Eum , A. Fantoni , G. Feofilov , J. Ferencei , F. Fichera , G. Fiorenza , A. N. Flores , A. Franco , M. Franco , J. P. Fransen , D. Gajanana , A. Galdames Perez , C. Gao , C. Gargiulo , L. Garizzo , P. Giubilato , M. Goffe , A. Grant , E. Grecka , L. Greiner , A. Grelli , A. Grimaldi , O. S. Groettvik , F. Grosa , C. Guo Hu , R. P. Hannigan , H. Helstrup , A. Hill , H. Hillemanns , P. Hindley , G. Huang , M. Iannone , J. P. Iddon , P. Ijzermans , M. A. Imhoff , A. Isakov , J. Jeong , T. Johnson , A. Junique , J. Kaewjai , M. Keil , Z. Khabanova , H. Khan , H. Kim , J. Kim , J. Kim , J. Kim , M. Kim , T. Kim , J. Klein , C. Kobdaj , A. Kotliarov , M. J. Kraan , I. Králik , F. Krizek , T. Kugathasan , C. Kuhn , P. G. Kuijer , S. Kushpil , M. J. Kweon , M. Kwon , Y. Kwon , P. La Rocca , N. Lacalamita , P. Larionov , G. Ledey , S. Lee , T. Lee , R. C. Lemmon , Y. Lesenechal , E. D. Lesser , B. E. Liang-Gilman , F. Librizzi , B. Lim , S. Lim , S. Lindsay , J. Liu , J. Liu , F. Loddo , M. Lupi , M. Mager , A. Maire , G. Mandaglio , V. Manzari , C. Markert , G. Markey , D. Marras , P. Martinengo , S. Martiradonna , M. Masera , A. Mastroserio , G. Mazza , D. Mazzaro , F. Mazzaschi , M. Mazzilli , L. Mcalpine , M. Mongelli , J. Morant , F. Morel , P. Morrall , V. Muccifora , A. Mulliri , L. Musa , A. I. Nambrath , M. Obergger , A. Orlandi , A. Palasciano , R. Panero , E. Paoletti , G. S. Pappalardo , O. Parasole , J. Park , L. Passamonti , C. Pastore , R. N. Patra , F. Pellegrino , A. Pepato , C. Petta , S. Piano , D. Pierluigi , S. Pisano , M. Pĺoskoń , M. T. Poblocki , S. Politano , E. Prakasa , F. Prino , M. Protsenko , M. Puccio , C. Puggioni , A. Rachevski , L. Ramello , M. Rasa , I. Ravasenga , A. U. Rehman , F. Reidt , M. Richter , F. Riggi , M. Rizzi , K. Røed , D. Röhrich , F. Ronchetti , M. J. Rossewij , A. Rossi , A. Russo , B. Di Ruzza , G. Saccà , M. Sacchetti , R. Sadikin , A. Sanchez Gonzalez , U. Savino , J. Schambach , F. Schlepper , R. Schotter , P. J. Secouet , M. Selina , S. Senyukov , J. J. Seo , R. Shahoyan , S. Shaukat , F. Shirokopetlev , K. Sielewicz , G. Simantovic , M. Sitta , R. J. M. Snellings , W. Snoeys , J. Song , J. M. Sonneveld , R. Spijkers , A. Sturniolo , C. P. Stylianidis , M. Šuljić , D. Sun , X. Sun , R. A. Syed , A. Szczepankiewicz , C. Terrevoli , M. Toppi , A. Trifiró , A. S. Triolo , S. Trogolo , V. Trubnikov , M. Turcato , R. Turrisi , T. Tveter , I. Tymchuk , G. L. Usai , V. Valentino , N. Valle , J. B. Van Beelen , J. W. Van Hoorne , T. Vanat , M. Varga-Kofarago , A. Velure , G. Venier , F. Veronese , A. Villani , A. Viticchié , C. Wabnitz , Y. Wang , P. Yang , E. R. Yeats , I. -K. Yoo , J. H. Yoon , S. Yuan , V. Zaccolo , A. Zampieri , C. Zampolli , E. Zhang , L. Zhang , X. Zhang , Z. Zhang , V. Zherebchevskii , N. Zurlo