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Pixel Detectors, as the current technology of choice for the innermost vertex detection, have reached a stage at which large detectors have been built for the LHC experiments and a new era of developments, both for hybrid and for monolithic…

Instrumentation and Detectors · Physics 2009-06-23 Norbert Wermes

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

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

For its physics program with a high-intensity hadron beam of up to 2e7 particles/s, the COMPASS experiment at CERN requires tracking of charged particles scattered by very small angles with respect to the incident beam direction. While good…

In high energy physics point to point resolution is a key prerequisite for particle detector pixel arrays. Current and future experiments require the development of inner-detectors able to resolve the tracks of particles down to the micron…

This paper covers the main technological and design aspects relevant to the development of a new generation of thin 3D pixel sensors with small pixel size aimed at the High-Luminosity LHC upgrades.

Plans to upgrade the LHC after approximately 10 years of operation are currently being considered at CERN. A tenfold increase in luminosity delivered to the experiments is envisaged in the so-called Super LHC (SLHC). This will undoubtedly…

Instrumentation and Detectors · Physics 2010-10-11 Stefanos Dris , Luis Amaral , Karl Gill , Robert Grabit , Alberto Pacheco , Daniel Ricci , Jan Troska , Francois Vasey

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…

While the CMS experiment is currently harvesting LHC collision data at CERN, the performance of its electromagnetic calorimeter (ECAL) is being constantly monitored, and work has started to assess the need for changes to the detector to…

Instrumentation and Detectors · Physics 2019-08-13 Francesca Nessi Tedaldi

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

The development of CMOS pixel sensors with column parallel read-out and integrated zero-suppression has resulted in a full size, nearly 1 Megapixel, prototype with ~100 \mu s read-out time. Its performances are quite close to the ILD vertex…

Instrumentation and Detectors · Physics 2010-07-16 Christine Hu-Guo , IPHC Collaboration , IRFU Collaboration

Silicon detectors based on the HV-CMOS technology are being investigated as possible candidate for the outer layers of the ATLAS pixel detector for the High Luminosity LHC. In this framework the H35Demo ASIC has been produced in the 350 nm…

Run-2 of the Large Hadron Collider (LHC) will provide new challenges to track and vertex reconstruction with higher energies, denser jets and higher rates. Therefore the ATLAS experiment has constructed the first 4-layer Pixel Detector in…

Instrumentation and Detectors · Physics 2016-08-30 Karolos Potamianos

HV-CMOS pixel sensors are a promising option for the tracker upgrade of the ATLAS experiment at the LHC, as well as for other future tracking applications in which large areas are to be instrumented with radiation-tolerant silicon pixel…

A precise and efficient tracking is one of the critical components of the CMS physics program as it impacts the ability to reconstruct the physics objects needed to understand proton-proton collisions at the LHC. The CMS detector has…

High Energy Physics - Experiment · Physics 2023-12-14 Walaa Elmetenawee

The Upgrade II of the LHCb detector, foreseen for 2031, will operate at an instantaneous luminosity of 1.5 x 10$^{34}$ cm$^{-2}$s$^{-1}$, accumulating a sample of more than 300 fb$^{-1}$. To cope with the estimated pile-up of 42 and 200…

Instrumentation and Detectors · Physics 2023-05-12 Evangelos Leonidas Gkougkousis

The LHCb experiment is designed to perform high-precision measurements of CP violation and search for New Physics using the enormous flux involving beauty and charm quarks produced at the LHC. The operation and the results obtained from the…

Instrumentation and Detectors · Physics 2013-10-02 Federico Alessio

The ATLAS experiment at the LHC will replace its current inner tracker system for the HL-LHC era. 3D silicon pixel sensors are being considered as radiation-hard candidates for the innermost layers of the new fully silicon-based tracking…

Instrumentation and Detectors · Physics 2019-09-04 S. Terzo , M. Chmeissani , G. Giannini , S. Grinstein , M. Manna , G. Pellegrini , D. Quirion , D. Vazquez Furelos

A prototype of the CMOS pixel sensor named SUPIX-1 has been fabricated and tested in order to investigate the feasibility of a pixelated tracker for a proposed Higgs factory, namely, the Circular Electron-Positron Collider (CEPC). The…

Instrumentation and Detectors · Physics 2022-01-05 L. Li , L. Zhang , J. N. Dong , J. Liu , M. Wang

The LHC is expected to reach luminosities up to 3000fb-1 and the innermost layer of the ATLAS upgrade plans to cope with higher occupancy and to decrease the pixel size. 3D-Si sensors are a good candidate for the innermost layer of the…

Instrumentation and Detectors · Physics 2017-03-08 Marta Baselga , Giulio Pellegrini , David Quirion