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Next generation Low Gain Avalanche Diodes (LGAD) produced by Hamamatsu photonics (HPK) and Fondazione Bruno Kessler (FBK) were tested before and after irradiation with ~1MeV neutrons at the JSI facility in Ljubljana. Sensors were irradiated…

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…

In this paper we report on a set of characterisations carried out on the first monolithic LGAD prototype integrated in a customised 110 nm CMOS process having a depleted active volume thickness of 48 $\mu$m. This prototype is formed by a…

The main purpose of this work is to provide reference data on X-ray ionization yields and energy spectra in liquid Ar to the studies in the field of Cryogenic Avalanche Detectors (CRADs) for rare-event and other experiments, based on liquid…

Instrumentation and Detectors · Physics 2016-02-19 A. Bondar , A. Buzulutskov , A. Dolgov , L. Shekhtman , A. Sokolov

The development of Low-Gain Avalanche Detectors has opened up the possibility of manufacturing silicon detectors with signal larger than that of traditional sensors. In this paper we explore the timing performance of Low-Gain Avalanche…

The temporal resolution of Low-Gain Avalanche Detectors (LGADs), also known as Ultra-Fast Silicon Detectors (UFSDs), is governed by two contributions: jitter, arising from electronic noise and signal slew rate, and the Landau noise term,…

High Energy Physics - Experiment · Physics 2026-03-12 N. Cartiglia , A. R. Altamura , R. Arcidiacono , M. Durando , S. Galletto , M. Ferrero , L. Lanteri , A. Losana , L. Massaccesi , L. Menzio , F. Siviero , V. Sola , R. White

Low Gain Avalanche Detectors (LGADs) are a type of thin silicon detector with a highly doped gain layer. LGADs manufactured by Fondazione Bruno Kessler (FBK) were tested before and after irradiation with neutrons. In this study, the…

LGAD technology is established within the field of particle physics, as the baseline technology for the timing detectors of both the ATLAS and CMS upgrades at the HL-LHC. Pixelated LGADs have been proposed for the High Granularity Timing…

Instrumentation and Detectors · Physics 2022-06-02 A. Doblas , D. Flores , S. Hidalgo , N. Moffat , G. Pellegrini , D. Quirion , J. Villegas , D. Maneuski , M. Ruat , P. Fajardo

A monolithic silicon pixel ASIC prototype, produced in 2024 as part of the Horizon 2020 MONOLITH ERC Advanced project, was tested with a 120 GeV/c pion beam. The ASIC features a matrix of hexagonal pixels with a 100 \mu m pitch, read by…

Studies of annealing at temperatures up to 450$^\circ$C with LGADs irradiated with neutrons are described. It was found that the performance of LGADs irradiated with 1.5e15 n/cm$^2$ was already improved at 5 minutes of annealing at…

Instrumentation and Detectors · Physics 2023-08-16 I. Mandić , V. Cindro , A. Gorišek , B. Hiti , A. Howard , Ž. Kljun , G. Kramberger , M. Maček Kržmanc , M. Mikuž , B. Novak

Hybrid pixel single-photon-counting detectors have been successfully employed and widely used in Synchrotron radiation X-ray detection. In this paper, the silicon pixel sensors for single X-ray photon detection, which operate in…

Instrumentation and Detectors · Physics 2016-08-03 Zhen-Jie Li , Yun-Cong Jia , Ling-Fei Hu , Peng Liu , Hua-Xiang Yin

This paper presents results that take a critical step toward proving 10 ps timing resolution's feasibility for particle identification in the TOPSiDE detector concept for the Electron-Ion Collider. Measurements of LGADs with a thickness of…

Instrumentation and Detectors · Physics 2021-07-07 M. Jadhav , W. Armstrong , I. Cloet , S. Joosten , S. M. Mazza , J. Metcalfe , Z. -E. Meziani , H. F. -W. Sadrozinski , B. Schumm , A. Seiden

Scintillation light produced in liquid xenon (LXe) by alpha particles, electrons and gamma-rays was detected with a large area avalanche photodiode (LAAPD) immersed in the liquid. The alpha scintillation yield was measured as a function of…

Instrumentation and Detectors · Physics 2009-11-11 K. Ni , E. Aprile , D. Day , K. L. Giboni , J. A. M. Lopes , P. Majewski , M. Yamashita

The presented study investigates the effects of low fluences from $5\times10^{12}$ up to $1\times10^{14}$ particles/cm$^{2}$ of 60MeV proton and neutron irradiation on n-type Low Gain Avalanche Detectors (nLGADs). An nLGAD is a silicon…

Instrumentation and Detectors · Physics 2025-08-11 Veronika Kraus , Marcos Fernandez Garcia , Salvador Hidalgo , Michael Moll , Jairo Villegas

Graphene integrated photonics provides several advantages over conventional Si photonics. Single layer graphene (SLG) enables fast, broadband, and energy-efficient electro-optic modulators, optical switches and photodetectors (GPDs), and is…

A closed-form approximate expression is presented for the short time-frame development of silicon diode sensor signals in the context of high frame-rate detection of incident X-ray fluxes, in the limit that the X-ray absorption profile…

Instrumentation and Detectors · Physics 2020-04-22 Bruce A. Schumm

We report on the design and performance of a mixed-signal application specific integrated circuit (ASIC) dedicated to avalanche photodiodes (APDs) in order to detect hard X-ray emissions in a wide energy band onboard the International Space…

Instrumentation and Methods for Astrophysics · Physics 2017-11-20 M. Arimoto , S. Harita , S. Sugita , Y. Yatsu , N. Kawai , H. Ikeda , H. Tomida , N. Isobe , S. Ueno , T. Mihara , M. Serino , T. Kohmura , T. Sakamoto , A. Yoshida , H. Tsunemi , S. Hatori , K. Kume , T. Hasegawa

The basic principle of operation of silicon sensors with resistive read-out is built-in charge sharing. Resistive Silicon Detectors (RSD, also known as AC-LGAD), exploiting the signals seen on the electrodes surrounding the impact point,…

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
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