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Monolithic Active Pixel Sensors (MAPS) achieved widespread use in several scientific applications, thanks to their properties, such as low material budget and high granularity. The ARCADIA INFN project developed a Fully-Depleted MAPS…

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…

This work presents a depleted monolithic active pixel sensor (DMAPS) prototype manufactured in the LFoundry 150\,nm CMOS process. DMAPS exploit high voltage and/or high resistivity inclusion of modern CMOS technologies to achieve…

This work presents a depleted monolithic active pixel sensor (DMAPS) prototype manufactured in the LFoundry 150 nm CMOS process. The described device, named LF-Monopix, was designed as a proof of concept of a fully monolithic sensor capable…

The Inner Tracking System (ITS) of the ALICE experiment at CERN will undergo an upgrade during the LHC long shutdown 3, in which the three innermost tracking layers will be replaced. This upgrade, named the Inner Tracking System 3 (ITS3),…

仪器与探测器 · 物理学 2023-12-14 M. Buckland

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…

仪器与探测器 · 物理学 2022-09-21 Bogdan-Mihail Blidaru

The paper presents the simulation studies of 10 $\mu$m pitch microstrips on a fully depleted monolithic active CMOS technology and describes their potential to provide a new and cost-effective solution for particle tracking and timing…

Monolithic Active Pixel Sensors (MAPS) have been developed since the late 1990s based on silicon substrates with a thin epitaxial layer (thickness of 10-15 $\mu$m) in which charge is collected on an electrode, albeit by disordered and slow…

Pixel detectors with cylindrical electrodes that penetrate the silicon substrate (so called 3D detectors) offer advantages over standard planar sensors in terms of radiation hardness, since the electrode distance is decoupled from the bulk…

A novel approach for designing the next generation of vertex detectors foresees to employ wafer-scale sensors that can be bent to truly cylindrical geometries after thinning them to thicknesses of 20-40$\mu$m. To solidify this concept, the…

仪器与探测器 · 物理学 2021-08-18 ALICE ITS project , : , G. Aglieri Rinella , M. Agnello , B. Alessandro , F. Agnese , R. S. Akram , J. Alme , E. Anderssen , D. Andreou , F. Antinori , N. Apadula , P. Atkinson , R. Baccomi , A. Badalà , A. Balbino , C. Bartels , R. Barthel , F. Baruffaldi , I. Belikov , S. Beole , P. Becht , A. Bhatti , M. Bhopal , N. Bianchi , M. B. Blidaru , G. Boca , J. Bok , G. Bonomi , M. Bonora , M. Borri , V. Borshchov , E. Botta , G. E. Bruno , M. Buckland , S. Bufalino , M. Cai , P. Camerini , P. Cariola , F. Catalano , C. Ceballos Sanchez , I. Chakaberia , M. Chartier , F. Colamaria , D. Colella , A. Collu , M. Concas , G. Contin , S. Costanza , P. Cui , A. Dainese , J. B. Dainton , L. De Cilladi , C. De Martin , G. De Robertis , W. Deng , A. Di Mauro , Y. Ding , M. Durkac , D. Elia , M. R. Ersdal , M. Faggin , F. Fan , A. Fantoni , P. Fecchio , A. Feliciello , G. Feofilov , A. Ferk , J. Ferencei , G. Fiorenza , A. N. Flores , E. Fragiacomo , D. Gajanana , A. Gal , C. Gao , C. Gargiulo , P. Gianotti , P. Giubilato , A. Grant , L. Greiner , A. Grelli , O. S. Groettvik , F. Grosa , C. Guo Hu , R. Hannigan , J. A. Hasenbichler , H. Helstrup , H. Hillemanns , C. Hills , P. Hindley , B. Hippolyte , B. Hofman , G. H. Hong , G. Huang , J. P. Iddon , H. Ilyas , M. A. Imhoff , A. Isakov , A. Jadlovska , S. Jadlovska , J. Jadlovsky , S. Jaelani , T. Johnson , A. Junique , P. Kalinak , A. Kalweit , M. Keil , Z. Khabanova , H. Khan , B. Kim , C. Kim , J. Kim , J. Kim , T. Kim , J. Klein , A. Kluge , C. Kobdaj , A. Kotliarov , I. Králik , F. Krizek , T. Kugathasan , C. Kuhn , P. G. Kuijer , S. Kushpil , M. J. Kweon , J. Y. Kwon , Y. Kwon , P. La Rocca , A. Lakrathok , R. Langoy , P. Larionov , E. Laudi , T. Lazareva , R. Lea , R. C. Lemmon , X. L. Li , J. Lien , B. Lim , S. H. Lim , S. Lindsay , A. Liu , J. Liu , J. Liu , M. Lunardon , G. Luparello , M. Lupi , M. Mager , A. Maire , Q. W. Malik , G. Mandaglio , V. Manzari , Y. Mao , G. V. Margagliotti , C. Markert , D. Marras , P. Martinengo , S. Masciocchi , M. Masera , A. Masoni , A. Mastroserio , P. F. T. Matuoka , G. Mazza , F. Mazzaschi , M. A. Mazzoni , F Morel , V. Muccifora , A. Mulliri , L. Musa , S. V. Nesbo , D. Nesterov , J. Norman , J. Park , R. N Patra , C. Pastore , H. Pei , X. Peng , S. Piano , C. Pinto , S. Pisano , S. Politano , E. Prakasa , F. Prino , M. Protsenko , M. Puccio , A. Rachevski , L. Ramello , F. Rami , I. Ravasenga , A. Rehman , F. Reidt , F. Riggi , K. Røed , D. Röhrich , F. Ronchetti , A. Rosano , M. J. Rossewij , A. Rossi , R. Rui , R. Russo , R. Sadikin , V. Sarritzu , J. Schambach , S. Senyukov , J. J. Seo , R. Shahoyan , S. Shaukat , S. Siddhanta , M. Sitta , R. J. M. Snellings , W. Snoeys , A. Songmoolnak , J. Sonneveld , F. Soramel , M. Suljic , S. Sumowidagdo , D. Sun , X. Sun , G. J. Tambave , G. Tersimonov , M. Tkacik , M. Toppi , A. Trifiró , S. Trogolo , V. Trubnikov , R. Turrisi , T. S. Tveter , I. Tymchuck , K. Ullaland , M. Urioni , G. L. Usai , N. Valle , L. V. R. van Doremalen , T. Vanat , J. W. Van Hoorne , M. Varga-Kofarago , A. Velure , D. Wang , Y. Wang , J. Wikne , J. R. Wright , R. Xu , P. Yang , Z. Yin , I. -K. Yoo , J. H. Yoon , S. Yuan , V. Zaccolo , E. Zhang , X. Zhang , V. Zherebchevskii , D. Zhou , J. Zhu , Y. Zhu , G. Zinovjev , N. Zurlo

The ATLAS Forward Physics (AFP) project plans to install 3D silicon pixel detectors about 210 m away from the interaction point and very close to the beamline (2-3 mm). This implies the need of slim edges of about 100-200 $\mu$m width for…

仪器与探测器 · 物理学 2015-11-09 Jörn Lange , Emanuele Cavallaro , Sebastian Grinstein , Ivan Lopez Paz

Depleted monolithic CMOS active pixel sensors (DMAPS) have been developed in order to demonstrate their suitability as pixel detectors in the outer layers of a toroidal LHC apparatus inner tracker (ATLAS ITk) pixel detector in the…

The Particle And Astrophysical Xenon Experiment III (PandaX-III) is an experiment to search for the Neutrinoless Double Beta Decay (NLDBD) using 200 kg radio-pure high-pressure gaseous xenon TPC with Micromegas detectors at both ends and…

仪器与探测器 · 物理学 2019-09-04 Danyang Zhu , Shubin Liu , Changqing Feng , Cheng Li , Haolei Chen

High Energy Particle Physics experiments at the LHC use hybrid silicon detectors, in both pixel and strip geometry, for their inner trackers. These detectors have proven to be very reliable and performant. Nevertheless, there is great…

The recent R&D focus on CMOS sensors with charge collection in a depleted zone has opened new perspectives for CMOS sensors as fast and radiation hard pixel devices. These sensors, labelled as depleted CMOS sensors (DMAPS), have already…

Depleted monolithic active pixel sensors (DMAPS), which exploit high voltage and/or high resistivity add-ons of modern CMOS technologies to achieve substantial depletion in the sensing volume, have proven to have high radiation tolerance…

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