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Related papers: The INFN-FBK Phase-2 R{\&}D Program

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The CMS experiment at the LHC includes a hybrid silicon pixel detector for the reconstruction of charged tracks and of the interaction vertices. The barrel region consists of n-in-n sensors with 100X150 um^2 cell size processed on diffusion…

The ITkPixV2 chip is the final production readout chip for the ATLAS Phase 2 Inner Tracker (ITk) upgrade at the upcoming High-Luminosity LHC (HL-LHC). Due to the extraordinarily high peak luminosity at the HL-LHC of $5 \times 10^{34}$…

Instrumentation and Detectors · Physics 2025-04-22 Luc Le Pottier , Timon Heim , Maurice Garcia-Sciveres

Between 2025 and 2027, some essential components of the CMS (Compact Muon Solenoid) detector - most notably the tracker and the calorimeter endcap - will be upgraded to prepare for HL-LHC (High Luminosity Large Hadron Collider) conditions.…

Instrumentation and Detectors · Physics 2020-03-26 Viktoria Hinger

The performance of pixel modules built from 75 micrometer thin silicon sensors and ATLAS read-out chips employing the Solid Liquid InterDiffusion (SLID) interconnection technology is presented. This technology, developed by the Fraunhofer…

Instrumentation and Detectors · Physics 2014-07-30 L. Andricek , M. Beimforde , A. Macchiolo , H-G. Moser , R. Nisius , R. H. Richter , S. Terzo , P. Weigell

The ALICE experiment is dedicated to the study of the quark gluon plasma in heavy-ion collisions at the CERN LHC. The Muon Forward Tracker (MFT) is under consideration by the ALICE experiment to be part of its program of detectors upgrade…

High Energy Physics - Experiment · Physics 2019-08-14 Antonio Uras

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

Fully Depleted Monolithic Active Pixels (FD-MAPS) represent a state-of-the-art detector technology and profit from a low material budget and cost for high energy physics experiments and other fields of research like medical imaging and…

Instrumentation and Detectors · Physics 2021-11-17 Coralie Neubüser , Thomas Corradino , Gian-Franco Dalla Betta , Lorenzo De Cilladi , Lucio Pancheri

The ALICE Collaboration is developing a novel vertexing detector to extend the heavy-flavour physics programme of the experiment during Run 4 by improving the pointing resolution of the tracking, particularly at low transverse momentum. It…

Instrumentation and Detectors · Physics 2024-08-05 Domenico Colella

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

DEPFET active pixel sensors are a well-developed technology for vertex detectors at future colliders. Extensive test beam campaigns have proven the excellent performance of these devices, and their radiation hardness has been thoroughly…

Instrumentation and Detectors · Physics 2019-08-13 Frank Simon

We have developed two radiation-hard ASICs for optical data transmission in the ATLAS pixel detector at the LHC at CERN: a driver chip for a Vertical Cavity Surface Emitting Laser (VCSEL) diode for 80 Mbit/s data transmission from the…

Instrumentation and Detectors · Physics 2017-08-23 K. K. Gan

The ARCADIA INFN R&D project developed a Fully Depleted Monolithic Active Pixel Sensor (FD-MAPS) using a customized LFoundry 110 nm CIS process. The first in-beam characterization of the ARCADIA Main Demonstrator 3 (MD3) sensor with 200…

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…

The use of CMOS Pixel Sensors (CPS) for high resolution and low material vertex detectors has been validated with the 2014 and 2015 physics runs of the STAR-PXL detector at RHIC/BNL. This opens the door to the use of CPS for inner tracking…

Instrumentation and Detectors · Physics 2017-03-08 A. Besson , A. Pérez Pérez , E. Spiriti , J. Baudot , G. Claus , M. Goffe , M. Winter

The ATLAS pixel detector is the innermost detector of the ATLAS experiment at the Large Hadron Collider at CERN. With approximately 80 million readout channels, the ATLAS silicon pixel detector is a high-acceptance, high-resolution,…

Instrumentation and Detectors · Physics 2019-08-13 E. Galyaev

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 present document discusses plans for a compact, next-generation multi-purpose detector at the LHC as a follow-up to the present ALICE experiment. The aim is to build a nearly massless barrel detector consisting of truly cylindrical…

Instrumentation and Detectors · Physics 2019-05-03 D. Adamová , G. Aglieri Rinella , M. Agnello , Z. Ahammed , D. Aleksandrov , A. Alici , A. Alkin , T. Alt , I. Altsybeev , D. Andreou , A. Andronic , F. Antinori , P. Antonioli , H. Appelshäuser , R. Arnaldi , I. C. Arsene , M. Arslandok , R. Averbeck , M. D. Azmi , X. Bai , R. Bailhache , R. Bala , L. Barioglio , G. G. Barnaföldi , L. S. Barnby , P. Bartalini , K. Barth , S. Basu , F. Becattini , C. Bedda , I. Belikov , F. Bellini , R. Bellwied , S. Beole , L. Bergmann , R. A. Bertens , M. Besoiu , L. Betev , A. Bhatti , A. Bianchi , L. Bianchi , J. Bielčík , J. Bielčíková , A. Bilandzic , S. Biswas , R. Biswas , D. Blau , F. Bock , M. Bombara , M. Borri , P. Braun-Munzinger , M. Bregant , G. E. Bruno , M. D. Buckland , H. Buesching , S. Bufalino , P. Buncic , J. B. Butt , A. Caliva , P. Camerini , F. Carnesecchi , J. Castillo Castellanos , F. Catalano , S. Chapeland , M. Chartier , C. Cheshkov , B. Cheynis , V. Chibante Barroso , D. D. Chinellato , P. Chochula , T. Chujo , C. Cicalo , F. Colamaria , D. Colella , M. Concas , Z. Conesa del Valle , G. Contin , J. G. Contreras , F. Costa , B. Dönigus , T. Dahms , A. Dainese , J. Dainton , A. Danu , S. Das , D. Das , S. Dash , A. Dash , G. David , A. De Caro , G. de Cataldo , A. De Falco , N. De Marco , S. De Pasquale , S. Deb , D. Di Bari , A. Di Mauro , T. Dietel , R. Divià , U. Dmitrieva , A. Dobrin , A. K. Dubey , A. Dubla , D. Elia , B. Erazmus , A. Erokhin , G. Eulisse , D. Evans , L. Fabbietti , M. Faggin , P. Fecchio , A. Feliciello , G. Feofilov , A. Fernández Téllez , A. Festanti , S. Floerchinger , P. Foka , S. Fokin , A. Franco , C. Furget , A. Furs , J. Gaardhøje , M. Gagliardi , P. Ganoti , C. Garabatos , E. Garcia-Solis , C. Gargiulo , P. Gasik , M. B. Gay Ducati , M. Germain , P. Ghosh , P. Giubellino , P. Giubilato , P. Glässel , V. Gonzalez , O. Grachov , A. Grigoryan , S. Grigoryan , F. Grosa , J. F. Grosse-Oetringhaus , R. Guernane , T. Gunji , R. Gupta , A. Gupta , M. K. Habib , H. Hamagaki , J. W. Harris , D. Hatzifotiadou , S. T. Heckel , E. Hellbär , H. Helstrup , T. Herman , H. Hillemanns , C. Hills , B. Hippolyte , S. Hornung , P. Hristov , J. P. Iddon , S. Igolkin , G. Innocenti , M. Ippolitov , M. Ivanov , A. Jacholkowski , M. Jung , A. Jusko , M. K. Köhler , S. Kabana , A. Kalweit , A. Karasu Uysal , T. Karavicheva , U. Kebschull , R. Keidel , M. Keil , B. Ketzer , S. A. Khan , A. Khanzadeev , Y. Kharlov , A. Khuntia , B. Kim , J. Kim , M. Kim , J. Klein , C. Klein , C. Klein-Bösing , S. Klewin , A. Kluge , M. L. Knichel , C. Kobdaj , M. Kofarago , P. J. Konopka , V. Kovalenko , I. Králik , M. Krüger , L. Kreis , M. Krivda , F. Krizek , M. Kroesen , E. Kryshen , V. Kučera , C. Kuhn , L. Kumar , S. Kundu , S. Kushpil , M. J. Kweon , M. Kwon , Y. Kwon , P. Lévai , S. L. La Pointe , E. Laudi , T. Lazareva , R. Lea , L. Leardini , S. Lee , R. C. Lemmon , R. Lietava , B. Lim , V. Lindenstruth , A. Lindner , C. Lippmann , J. Liu , J. Lopez Lopez , C. Lourenco , G. Luparello , S. M. Mahmood , A. Maire , V. Manzari , Y. Mao , A. Marín , M. Marchisone , G. V. Margagliotti , M. Marquard , P. Martinengo , S. Masciocchi , M. Masera , E. Masson , A. Mastroserio , A. M. Mathis , A. Matyja , M. Mazzilli , M. A. Mazzoni , L. Micheletti , A. N. Mishra , D. Miskowiec , B. Mohanty , M. Mohisin Khan , A. Morsch , T. Mrnjavac , V. Muccifora , D. Mühlheim , S. Muhuri , J. D. Mulligan , M. G. Munhoz , R. H. Munzer , H. Murakami , L. Musa , B. Naik , B. K. Nandi , R. Nania , T. K. Nayak , D. Nesterov , G. Nicosia , S. Nikolaev , V. Nikulin , F. Noferini , J. Norman , A. Nyanin , V. Okorokov , C. Oppedisano , J. Otwinowski , K. Oyama , M. Płoskoń , Y. Pachmayer , A. K. Pandey , C. Pastore , J. Pawlowski , H. Pei , T. Peitzmann , D. Peresunko , M. Petrovici , R. P. Pezzi , S. Piano , E. Prakasa , S. K. Prasad , R. Preghenella , F. Prino , C. A. Pruneau , I. Pshenichnov , M. Puccio , J. Pucek , E. Quercigh , D. Röhrich , L. Ramello , F. Rami , S. Raniwala , R. Raniwala , R. Rath , I. Ravasenga , A. Redelbach , K. Redlich , F. Reidt , K. Reygers , V. Riabov , P. Riedler , W. Riegler , D. Rischke , C. Ristea , S. P. Rode , M. Rodríguez Cahuantzi , D. Rohr , A. Rossi , R. Rui , A. Rustamov , A. Rybicki , K. Šafařík , R. Sadikin , S. Sadovsky , R. Sahoo , P. Sahoo , P. K. Sahu , J. Saini , V. Samsonov , P. Sarma , H. S. Scheid , R. Schicker , A. Schmah , M. O. Schmidt , C. Schmidt , Y. Schutz , K. Schweda , E. Scomparin , J. E. Seger , S. Senyukov , A. Seryakov , R. Shahoyan , N. Sharma , S. Siddhanta , T. Siemiarczuk , R. Singh , M. Sitta , H. Soltveit , M. Spyropoulou-Stassinaki , J. Stachel , T. Sugitate , S. Sumowidagdo , X. Sun , J. Takahashi , C. Terrevoli , A. Toia , N. Topilskaya , S. Tripathy , S. Trogolo , V. Trubnikov , W. H. Trzaska , B. A. Trzeciak , T. S. Tveter , A. Uras , G. L. Usai , G. Valentino , L. V. R. van Doremalen , M. van Leeuwen , P. Vande Vyvre , M. Vasileiou , V. Vechernin , L. Vermunt , O. Villalobos Baillie , T. Virgili , A. Vodopyanov , S. A. Voloshin , G. Volpe , B. von Haller , I. Vorobyev , Y. Wang , M. Weber , A. Wegrzynek , D. F. Weiser , S. C. Wenzel , J. P. Wessels , J. Wiechula , U. Wiedemann , J. Wilkinson , B. Windelband , M. Winn , N. Xu , K. Yamakawa , Z. Yin , I. -K. Yoo , J. H. Yoon , A. Yuncu , V. Zaccolo , C. Zampolli , A. Zarochentsev , B. Zhang , X. Zhang , C. Zhao , V. Zherebchevskii , D. Zhou , Y. Zhou , Y. Zhou , G. Zinovjev

Results obtained with 3D columnar pixel sensors bump-bonded to the RD53A prototype readout chip are reported. The interconnected modules have been tested in a hadron beam before and after irradiation to a fluence of about…

The ATLAS Pixel detector is a high-resolution, low-noise silicon-based device designed to provide tracking and vertexing information within a distance of 12 cm from the LHC beam axis. It consists of approximately 80 million pixel channels…

Instrumentation and Detectors · Physics 2019-08-13 J. Biesiada

Depleted Monolithic Active Pixel Sensors (DMAPS) constitute a promising low cost alternative for the outer layers of the ATLAS experiment Inner Tracker (ITk). Realizations in modern, high resistivity CMOS technologies enhance their…