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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…

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

This paper presents the principles of operation of Resistive AC-Coupled Silicon Detectors (RSDs) and measurements of the temporal and spatial resolutions using a combined analysis of laser and beam test data. RSDs are a new type of n-in-p…

We report on the successful operation of a double phase Liquid Argon Large Electron Multiplier Time Projection Chamber (LAr LEM-TPC) equipped with two dimensional projective anodes with dimensions 10$\times$10 cm$^2$, and with a maximum…

Instrumentation and Detectors · Physics 2015-06-18 C. Cantini , L. Epprecht , A. Gendotti , S. Horikawa , S. Murphy , G. Natterer , L. Periale , F. Resnati , A. Rubbia , F. Sergiampietri , T. Viant , S. Wu

Detectors based on pixels with timing capabilities are gaining increasing importance in the last years. Next-to-come high-energy physics experiments at colliders requires the use of time information in tracking, due to the increasing levels…

Instrumentation and Detectors · Physics 2020-08-25 Adriano Lai , Gian Matteo Cossu

The planned luminosity increase at the Large Hadron Collider in the coming years has triggered interest in the use of the particles' time of arrival as additional information in specialized detectors to mitigate the impact of pile-up. The…

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

A micro-pulse lidar at eye-safe wavelength is constructed based on an up-conversion single-photon detector. The ultralow noise detector enables using integration technique to improve the signal-to-noise ratio of the atmospheric…

The concept of capacitive coupling between sensors and readout chips is under study for the vertex detector at the proposed high-energy CLIC electron positron collider. The CLICpix Capacitively Coupled Pixel Detector (C3PD) is an active…

Instrumentation and Detectors · Physics 2017-10-06 I. Kremastiotis , R. Ballabriga , M. Campbell , D. Dannheim , A. Fiergolski , D. Hynds , S. Kulis , I. Peric

In this radiation tolerance study, Low Gain Avalanche Detectors (LGADs) with a carbon-enriched broad and shallow multiplication layer were examined in comparison to identical non-carbonated LGADs. Manufactured at IMB-CNM, the sensors…

Low Gain Avalanche Detectors (LGAD) represent a remarkable advance in high energy particle detection, since they provide a moderate increase (gain ~10) of the collected charge, thus leading to a notable improvement of the signal-to-noise…

Instrumentation and Detectors · Physics 2016-05-04 Pablo Fernandez-Martinez , David Flores , Salvador Hidalgo , Virginia Greco , Angel Merlos , Giulio Pellegrini , David Quirion

High-Voltage Monolithic Active Pixel Sensors (HV-MAPS) based on the 180 nm HV-CMOS process have been proposed to realize thin, fast and highly integrated pixel sensors. The MuPix7 prototype, fabricated in the commercial AMS H18 process,…

LF-Monopix1 and TJ-Monopix1 are depleted monolithic active pixel sensors (DMAPS) in 150 nm LFoundry and 180 nm TowerJazz CMOS technologies respectively. They are designed for usage in high-rate and high-radiation environments such as the…

Using the maximum-likelihood detector (MLD) of a soliton with timing jitter and noise, other than walk-out of the bit interval, timing jitter does not degrade the performance of MLD. When the MLD is simulated with important sampling method,…

Optics · Physics 2013-01-15 Keang-Po Ho

The High Granularity Timing Detector (HGTD) will be installed in the ATLAS experiment as part of the Phase-II upgrade for the High Luminosity-Large Hadron Collider (HL-LHC). It will mitigate pile-up effects in the forward region, and…

Instrumentation and Detectors · Physics 2026-02-02 A. Aboulhorma , M. Ait Tamlihat , H. M. Alfanda , O. Atanova , N. Atanov , I. Azzouzi , J. Barreiro Guimarães da Costa , T. Beau , D. Benchekroun , F. Bendebba , G. Bergamin , Y. Bimgdi , A. Blot , A. Boikov , J. Bonis , D. Boumediene , C. Brito , A. S. Brogna , A. M. Burger , L. Cadamuro , Y. Cai , N. Cartalade , R. Casanova Mohr , R. Cherkaoui El Moursli , Y. Che , X. Chen , E. Y. S. Chow , L. D. Corpe , C. G. Crozatier , L. D'Eramo , S. Dahbi , D. Dannheim , G. Daubard , Y. Davydov , J. Debevc , Y. Degerli , E. Delagnes , F. Deliot , M. Dhellot , P. Dinaucourt , G. Di Gregorio , P. J. Dos Santos De Assis , C. Duan , O. Duarte , F. Dulucq , J. Ehrecke , Y. El Ghazali , A. El Moussaouy , A. Falou , L. Fan , Y. Fan , Z. Fan , K. Farman , F. Fassi , Y. Feng , M. Ferreira , F. Filthaut , F. Fischer , P. Fusté , J. Fu , J. García Rodriquez , G. Gaspar De Andrade , V. Gautam , Z. Ge , R. Gonçalo , M. Gouighri , S. Grinstein , K. Gritsay , F. Guilloux , S. Guindon , A. Haddad , S. E. D. Hammoud , L. Han , A. M. Henriques Correia , M. Hidaoui , B. Hiti , J. Hofner , S. Hou , P. J. Hsu , X. Huang , Y. Huang , K. Hu , C. Insa , J. Jeglot , X. Jia , G. Kramberger , M. Kuriyama , B. Y. Ky , D. Lacour , A. Lafarge , B. Lakssir , A. Lantheaume , D. Laporte , C. de La Taille , M. A. L. Leite , A. Leopold , H. Li , L. Li , M. Li , S. Li , S. Li , Y. Li , Z. Li , S. Liang , Z. Liang , B. Liu , K. Liu , K. Liu , Y. L. Liu , Y. W. Liu , F. L. Lucio Alves , M. Lu , Y. J. Lu , F. Lyu , D. Macina , R. Madar , N. Makovec , S. Malyukov , I. Mandić , T. Manoussos , S. Manzoni , G. Martin-Chassard , F. Martins , L. Masetti , R. Mazini , E. Mazzeo , K. Ma , X. Ma , R. Menegasso , J-P. Meyer , Y. Miao , A. Migayron , M. Mihovilovic , M. Milovanovic , M. Missio , V. Moskalenko , N. Mouadili , A. Moussa , I. Nikolic-Audit , C. C. Ohm , H. Okawa , S. Okkerman , M. Ouchrif , C. Pénélaud , A. Parreira , B. Pascual Dias , R. E. de Paula , J. Pinol Bel , P. -O. Puhl , C. Puigdengoles Olive , M. Puklavec , J. Qin , M. Qi , H. Ren , H. Riani , S. Ridouani , V. Rogozin , L. Royer , F. Rudnyckyj , E. F. Saad , G. T. Saito , A. Salem , H. Santos , S. Scarfi , Ph. Schwemling , N. Seguin-Moreau , L. Serin , R. P. Serrano Fernandez , A. Shaikovskii , Q. Sha , L. Shan , R. Shen , X. Shi , P. Skomina , H. Smitmanns , H. L. Snoek , A. P. Soulier , A. Stein , H. Stenzel , J. Strandberg , W. Sun , X. Sun , Y. Sun , Y. Tan , K. Tariq , Y. Tayalati , S. Terzo , A. Torrento Coello , S. Trincaz-Duvoid , U. M. Vande Voorde , I. Velkovska , R. P. Vieira , L. A. Vieira Lopes , A. Visibile , A. Wang , C. Wang , S. M. Wang , T. Wang , T. Wang , W. Wang , Y. Wang , Y. Wang , J. Wan , Q. Weitzel , J. Wu , M. Wu , W. Wu , Y. Wu , L. Xia , D. Xu , H. Xu , L. Xu , Z. Yan , H. Yang , H. Yang , X. Yang , X. Yang , J. Ye , I. Youbi , J. Yuan , I. Zahir , H. Zeng , D. Zhang , J. Zhang , L. Zhang , Z. Zhang , M. Zhao , Z. Zhao , X. Zheng , Z. Zhou , Y. Zhu , X. Zhuang

We show the developments carried out to improve the silicon sensor technology for the detection of soft X-rays with hybrid X-ray detectors. An optimization of the entrance window technology is required to improve the quantum efficiency. The…

InGaAs/InP single-photon avalanche diodes (SPADs) working in the regime of GHz clock rates are crucial components for the high-speed quantum key distribution (QKD). We have developed for the first time a compact, stable and user-friendly…

Quantum Physics · Physics 2015-06-05 Xiao-Lei Liang , Jian-Hong Liu , Quan Wang , De-Bing Du , Jian Ma , Ge Jin , Zeng-Bing Chen , Jun Zhang , Jian-Wei Pan

This paper presents the design and results of detailed tests of a CMOS active pixel chip for charged particle detection with in-pixel charge storage for correlated double sampling and readout in rolling shutter mode at frequencies up to 25…

Instrumentation and Detectors · Physics 2009-01-27 Marco Battaglia , Jean-Marie Bussat , Devis Contarato , Peter Denes , Piero Giubilato , Lindsay E. Glesener

The SoLID spectrometer's gas Cherenkov counters require photosensors that operate in a high luminosity and high background environment. The reference design features arrays of 9 or 16 tiled multi-anode photomultipliers (MaPMTs), distributed…

During the High Luminosity phase of LHC, up to 200 proton-proton collisions per bunch crossing will bring severe challenges for event reconstruction. To mitigate pileup effects, an extended upgrade program of the CMS experiment is expected.…

High Energy Physics - Experiment · Physics 2026-03-23 Simona Palluotto