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In the LHC long shutdown 3, the ALICE experiment upgrades the inner layers of its Inner Tracker System with three layers of wafer-scale stitched sensors bent around the beam pipe. Two stitched sensor evaluation structures, the MOnolithic…

We present the first physical realization of in-pixel signal processing with integrated AI-based data filtering for particle tracking detectors. Building on prior work that demonstrated a physics-motivated edge-AI algorithm suitable for…

The development of an innovative position sensitive pixelated sensor to detect and measure with high precision the coordinates of the ionizing particles is proposed. The silicon avalanche pixel sensors (APiX) is based on the vertical…

Instrumentation and Detectors · Physics 2015-06-18 N. D'Ascenzo , P. S. Marrocchesi , C. S. Moon , F. Morsani , L. Ratti , V. Saveliev , A. Savoy Navarro , Q. Xie

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…

The Inner Tracking System is the ALICE detector closest to the beam axis. It is composed of six layers of silicon detectors: two innermost layers of Silicon Pixel Detectors (SPD), two intermediate layers of Silicon Drift Detectors (SDD) and…

Instrumentation and Detectors · Physics 2019-08-14 L. Milano

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

The technological prototype of the CALICE highly granular silicon-tungsten electromagnetic calorimeter (SiW-ECAL) was tested in a beam at DESY in 2017. The setup comprised seven layers of silicon sensors. Each layer comprised four sensors,…

In next ten years, the Large Hadron Collider will be upgraded to the High Luminosity LHC (HL-LHC), resulting in ten time more integrated luminosity. To withstand the much harsher radiation and occupancy conditions of the HL-LHC, the inner…

Instrumentation and Detectors · Physics 2019-05-01 Zhijun Liang

Pixel sensors based on commercial high-voltage CMOS processes are an exciting technology that is considered as an option for the outer layer of the ATLAS inner tracker upgrade at the High Luminosity LHC. Here, charged particles are detected…

The ALICE experiment at CERN is undergoing a major upgrade during the Long Shutdown 2 (LS2) of the LHC during 2019-2020. The key elements regarding the central barrel are the installation of a new Inner Tracking System (ITS) and the upgrade…

Instrumentation and Detectors · Physics 2021-02-03 Felix Reidt

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

To cope with the High Luminosity LHC harsh conditions, the ATLAS inner tracker has to be upgraded to meet requirements in terms of radiation hardness, pile up and geometrical acceptance. The active edge technology allows to reduce the…

The 3D silicon sensor has demonstrated excellent performances (signal collection, detection efficiency, power consumption, etc.) comparable or even better with respect to the traditional planar sensor of the ATLAS Detector at the Large…

The apparatus of the ALICE experiment at CERN will be upgraded in 2017/18 during the second long shutdown of the LHC (LS2). A major motivation for this upgrade is to extend the physics reach for charmed and beauty particles down to low…

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

For the High Luminosity upgrade of the Large Hadron Collider the current ATLAS Inner Detector will be replaced by an all-silicon Inner Tracker. The pixel detector will consist of five barrel layers and a number of rings, resulting in about…

Instrumentation and Detectors · Physics 2021-05-24 Lingxin Meng

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

The physics aims at the proposed future high-energy linear $e^+e^-$ collider CLIC pose challenging demands on the performance of the detector system. In particular, the vertex and tracking detectors have to combine a spatial resolution of a…

Instrumentation and Detectors · Physics 2020-10-22 Katharina Dort

A testbeam telescope, based on ATLAS IBL silicon pixel modules, has been built. It comprises six planes of planar silicon sensors with 250 x 50 um^2 pitch, read out by ATLAS FE-I4 chips. In the CERN SPS H8 beamline (180 GeV pi+) a…

A demonstrator for each slice of the ATLAS pixel detector was built to replicate the real detector and provide early solutions for operating and maintaining its components. This system-level testing of the all-silicon Inner Tracker (ITk)…

High Energy Physics - Experiment · Physics 2025-01-15 Yahya Khwaira
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