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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

The characterization of spacial and timing resolution of the novel Trench Isolated LGAD (TI-LGAD) technology is presented. This technology has been developed at FBK with the goal of achieving 4D pixels, where an accurate position resolution…

Gain-layer degradation from exposure to radiation limits the use of Low-Gain Avalanche Diodes (LGADs) in high energy particle physics detector experiments. Proper understanding of how the gain-layer is destroyed is not available on a defect…

It is well known that avalanche photodiodes operated in the Geiger mode above the breakdown voltage offer a virtually infinite sensitivity and time accuracy in the picosecond range that can be used for single photon detection. However,…

Instrumentation and Detectors · Physics 2012-01-30 E. Vilella , O. Alonso , J. Trenado , A. Vilà , M. Vos , L. Garrido , A. Diéguez

In recent years, the gain suppression mechanism has been studied for large localized charge deposits in Low-Gain Avalanche Detectors (LGADs). LGADs are a thin silicon detector with a highly doped gain layer that provides moderate internal…

Recent interest in pile-up mitigation through fast timing at the HL-LHC has focused attention on technologies that now achieve minimum ionising particle (MIP) time resolution of 30 picoseconds or less. The constraints of technical maturity…

Instrumentation and Detectors · Physics 2019-10-18 M. Centis Vignali , M. Gallinaro , B. Harrop , C. Lu , M. McClish , M. Moll , M. Newcomer , S. Otero Ugobono , S. White

The 4H-SiC material exhibits good detection performance, but there are still many problems like signal distortion and poor signal quality. The 4H-SiC low gain avalanche detector (LGAD) has been fabricated for the first time to solve these…

Instrumentation and Detectors · Physics 2024-05-29 Sen Zhao , Keqi Wang , Kaibo Xie , Chenxi Fu , Chengwei Wang , Xin Shi , Congcong Wang

We propose a joint TDC and multi-time-gated imaging single-photon avalanche diode LiDAR sensor featuring a maximum detection range of 108m with a minimum depth resolution (least significant bit) of 2.93mm, fabricated in 110nm CMOS…

Optics · Physics 2026-03-23 Chang Liu , Edoardo Charbon

Low-Gain Avalanche Detectors (LGADs) are the leading 4D sensing technology selected for use in the High Luminosity Large Hadron Collider (HL-LHC). However, their proximity to the interaction point makes them highly susceptible to…

Instrumentation and Detectors · Physics 2025-06-23 Rajiv Gupta , Sunidhi Saxena , Kalpna Tiwari , Rahul Sharma , Namrata Agrawal , Ashutosh Bhardwaj , Kirti Ranjan , Ajay Kumar

The development of detectors that provide high resolution in four dimensions has attracted wide-spread interest in the scientific community for applications in high-energy physics, nuclear physics, medical imaging, mass spectroscopy as well…

The increasing concentration of greenhouse gases, notably CH4 and CO2, has fueled global temperature increases, intensifying concerns regarding the prevailing climate crisis. Effectively monitoring these gases demands a detector spanning…

The development of CMOS pixel sensors with column parallel read-out and integrated zero-suppression has resulted in a full size, nearly 1 Megapixel, prototype with ~100 \mu s read-out time. Its performances are quite close to the ILD vertex…

Instrumentation and Detectors · Physics 2010-07-16 Christine Hu-Guo , IPHC Collaboration , IRFU Collaboration

The ATLAS experiment will undergo around the year 2025 a replacement of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) with a new 5-layer pixel system. Thin planar pixel sensors are promising candidates to…

Instrumentation and Detectors · Physics 2017-02-01 Anna Macchiolo , Julien Beyer , Alessandro La Rosa , Richard Nisius , Natascha Savic

Resistive AC-coupled Silicon Detectors (RSDs) are based on the Low Gain Avalanche Diode (LGAD) technology, characterized by a continuous gain layer, and by the innovative introduction of resistive read-out. Thanks to a novel electrode…

High-resolution 3D tracking with sub-nanosecond timing is required for the detection of elementary particles, such as neutrinos. Conventional detectors, which utilize analog silicon photomultipliers, face challenges in balancing spatial…

Instrumentation and Detectors · Physics 2025-11-24 Kodai Kaneyasu , Till Dieminger , Matthew Franks , Davide Sgalaberna , Claudio Bruschini , Edoardo Charbon

This paper describes the new concept of the double-LGAD. The goal is to increase the charge at the input of the electronics, keeping a time resolution equal or better than a standard (single) LGAD; this has been realized by adding the…

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,…

We present a novel approach to implement compressive sensing in laser scanning microscopes (LSM), specifically in image scanning microscopy (ISM), using a single-photon avalanche diode (SPAD) array detector. Our method addresses two…

Image and Video Processing · Electrical Eng. & Systems 2023-07-20 Ajay Gunalan , Marco Castello , Simonluca Piazza , Shunlei Li , Alberto Diaspro , Leonardo S. Mattos , Paolo Bianchini

Owing to their intrinsic (geometry dependent) radiation hardness, 3D pixel sensors are promising candidates for the innermost tracking layers of the forthcoming experiment upgrades at the Phase 2 High-Luminosity LHC (HL-LHC). To this…

Instrumentation and Detectors · Physics 2017-02-01 DMS Sultan , Gian-Franco Dalla Betta , Roberto Mendicino , Maurizio Boscardin , Sabina Ronchin , Nicola Zorzi

The response of Low Gain Avalanche Diodes (LGADs), a type of thin silicon detector with internal gain, to X-rays of energies between 6-16~keV was characterized at the Stanford Synchrotron Radiation Lightsource (SSRL). The utilized beamline…

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