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The Topmetal-M is a large area pixel sensor (18 mm * 23 mm) prototype fabricated in a new 130 nm high-resistivity CMOS process in 2019. It contains 400 rows * 512 columns square pixels with the pitch of 40 {\mu}m. In Topmetal-M, a novel…

XRPIX is the monolithic X-ray SOI (silicon-on-insulator) pixel detector, which has a time resolution better than 10 $\rm{\mu}$s as well as a high detection efficiency for X-rays above 10 keV. XRPIX is planned to be installed on future X-ray…

The precise reconstruction of Compton-scatter events is paramount for an imaging medium-energy gamma-ray telescope. The proposed AMEGO-X is enabled by a silicon tracker utilizing AstroPix chips - a pixelated silicon HVCMOS sensor novel for…

Single electron Sensitive Read Out (SiSeRO) is a novel on-chip charge detector output stage for charge-coupled device (CCD) image sensors. Developed at MIT Lincoln Laboratory, this technology uses a p-MOSFET transistor with a depleted…

This paper presents the results of the characterisation of a pixel sensor manufactured in OKI 0.2 micron SOI technology integrated on a high-resistivity substrate, and featuring several pixel cell layouts for charge collection optimisation.…

Instrumentation and Detectors · Physics 2011-10-19 Marco Battaglia , Dario Bisello , Devis Contarato , Peter Denes , Piero Giubilato , Serena Mattiazzo , Devis Pantano , Sarah Zalusky

3D silicon pixel detectors have been investigated as radiation-hard candidates for the innermost layers of the HL-LHC upgrade of the ATLAS pixel detector. 3D detectors are already in use today in the ATLAS IBL and AFP experiments. These are…

A silicon 3D detector with a single cell of 50x50 um2 was produced and evaluated for timing applications. The measurements of time resolution were performed for 90Sr electrons with dedicated electronics used also for determining time…

Instrumentation and Detectors · Physics 2019-06-26 G. Kramberger , V. Cindro , D. Flores , S. Hidalgo , B. Hiti , M. Manna , I. Mandić , M. Mikuž , D. Quirion , G. Pellegrini , M. Zavrtanik

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…

We present a gated silicon single photon detector based on a commercially available avalanche photodiode. Our detector achieves a photon detection efficiency of 45\pm5% at 808 nm with 2x 10^-6 dark count per ns at -30V of excess bias and…

Instrumentation and Detectors · Physics 2015-06-11 T. Lunghi , E. Pomarico , C. Barreiro , D. Stucki , B. Sanguinetti , H. Zbinden

Using the simulation framework of the SiD detector to study the Higgs -> mumu decay channel showed a considerable gain in signal significance could be achieved through an increase in charged particle momentum resolution. However more…

Instrumentation and Detectors · Physics 2011-04-26 T. G. White

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

For experiments at the European X-Ray Free-Electron Laser (XFEL) the Adaptive Gain Integrating Pixel Detector (AGIPD) is under development. The particular requirements for the detector are a high dynamic range of 0, 1 - to more than 10E4…

Instrumentation and Detectors · Physics 2015-06-11 J. Schwandt , E. Fretwurst , R. Klanner , J. Zhang

High-granularity homogeneous electromagnetic calorimeters based on scintillating crystals and silicon photomultipliers (SiPMs) are a promising option for future $e^{+}e^{-}$ Higgs factories, where both excellent energy resolution and a very…

Instrumentation and Detectors · Physics 2026-03-10 Zhiyu Zhao , Dejing Du , Shu Li , Yong Liu , Baohua Qi , Jack Rolph , Haijun Yang

Dynamic x-ray studies may reach temporal resolutions limited by only the x-ray pulse duration if the detector is fast enough to segregate synchrotron pulses. An analog integrating pixel array detector with in-pixel storage and temporal…

Instrumentation and Detectors · Physics 2010-07-28 Lucas J. Koerner , Sol M. Gruner

We present a 'digital SiPM' photo-detection chip combining single photon sensitive avalanche photo diodes and CMOS readout electronics on a single die. The chip has a size of $8046\times9032\,\mu m^2$ with $72.5\%$ of photo sensitive area.…

Instrumentation and Detectors · Physics 2025-01-27 Peter Fischer , Michael Keller , Michael Ritzert

This paper presents the results of the characterisation of a thin, fully depleted pixel sensor manufactured in SOI technology on high-resistivity substrate with high momentum charged particles. The sensor is thinned to 70 $\mu$m and a thin…

Instrumentation and Detectors · Physics 2012-02-17 Marco Battaglia , Dario Bisello , Devis Contarato , Peter Denes , Piero Giubilato , Serena Mattiazzo , Devis Pantano

The MIP Timing Detector will provide additional timing capabilities for detection of minimum ionizing particles (MIPs) at CMS during the High Luminosity LHC era, improving event reconstruction and pileup rejection. The central portion of…

Instrumentation and Detectors · Physics 2021-07-19 R. Abbott , A. Abreu , F. Addesa , M. Alhusseini , T. Anderson , Y. Andreev , A. Apresyan , R. Arcidiacono , M. Arenton , E. Auffray , D. Bastos , L. A. T. Bauerdick , R. Bellan , M. Bellato , A. Benaglia , M. Benettoni , R. Bertoni , M. Besancon , S. Bharthuar , A. Bornheim , E. Brücken , J. N. Butler , C. Campagnari , M. Campana , R. Carlin , P. Carniti , N. Cartiglia , M. Casarsa , O. Cerri , P. Checchia , H. Chen , S. Chidzik , F. Chlebana , F. Cossutti , M. Costa , B. Cox , I. Dafinei , F. De Guio , P. Debbins , D. del Re , A. Dermenev , E. Di Marco , K. Dilsiz , K. F. Di Petrillo , G. Dissertori , S. Dogra , U. Dosselli , I. Dutta , F. Caleb , C. Fernandez Madrazo , M. Fernandez , M. Ferrero , Z. Flowers , W. Funk , M. Gallinaro , S. Ganjour , M. Gardner , F. Geurts , A. Ghezzi , S. Gninenko , F. Golf , J. Gonzalez , C. Gotti , L. Gray , F. Guilloux , S. Gundacker , E. Hazen , S. Hedia , A. Heering , R. Heller , T. Isidori , R. Isocrate , R. Jaramillo , M. Joyce , K. Kaadze , A. Karneyeu , H. Kim , J. King , G. Kopp , M. Korjik , O. K. Koseyan , A. Kozyrev , N. Kratochwil , M. Lazarovits , A. Ledovskoy , H. Lee , J. Lee , A. Li , S. Li , W. Li , T. Liu , N. Lu , M. Lucchini , W. Lustermann , C. Madrid , M. Malberti , I. Mandjavize , J. Mao , Y. Maravin , D. Marlow , B. Marsh , P. Martinez del Arbol , B. Marzocchi , R. Mazza , C. McMahon , V. Mechinsky , P. Meridiani , A. Mestvirishvili , N. Minafra , A. Mohammadi , F. Monti , C. S. Moon , R. Mulargia , M. Murray , Y. Musienko , J. Nachtman , S. Nargelas , L. Narvaez , O. Neogi , C. Neu , T. Niknejad , M. Obertino , H. Ogul , G. Oh , I. Ojalvo , Y. Onel , G. Organtini , T. Orimoto , J. Ott , I. Ovtin , M. Paganoni , F. Pandolfi , R. Paramatti , A. Peck , C. Perez , G. Pessina , C. Pena , S. Pigazzini , O. Radchenko , N. Redaelli , D. Rigoni , E. Robutti , C. Rogan , R. Rossin , C. Rovelli , C. Royon , M. Ö. Sahin , W. Sands , F. Santanastasio , U. Sarica , I. Schmidt , R. Schmitz , J. Sheplock , J. C. Silva , F. Siviero , L. Soffi , V. Sola , G. Sorrentino , M. Spiropulu , D. Spitzbart , A. G. Stahl Leiton , A. Staiano , D. Stuart , I. Suarez , T. Tabarelli de Fatis , G. Tamulaitis , Y. Tang , B. Tannenwald , R. Taylor , E. Tiras , M. Titov , S. Tkaczyk , D. Tlisov , I. Tlisova , M. Tornago , M. Tosi , R. Tramontano , J. Trevor , C. G. Tully , B. Ujvari , J. Varela , S. Ventura , I. Vila , T. Wamorkar , C. Wang , X. Wang , M. Wayne , J. Wetzel , S. White , D. Winn , S. Wu , S. Xie , Z. Ye , G. B. Yu , G. Zhang , L. Zhang , Y. Zhang , Z. Zhang , R. Zhu

The SAMpler for PICosecond time (SAMPIC) chip has been designed by a collaboration including CEA/IRFU/SEDI, Saclay and CNRS/LAL/SERDI, Orsay. It benefits from both the quick response of a time to digital converter and the versatility of a…

Dense tracking environments in experiments at CERN's High-Luminosity LHC and future FCC experiments call for an increased use of timing information in addition to the position measurement of pixel detectors. This adds one dimension to the…

On-chip integration of two-dimensional (2D) materials offers great potential for the realization of novel optoelectronic devices in different photonic platforms. In particular, indium selenide (InSe) is a very promising 2D material due to…