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We report on the status and development of polarization-sensitive detectors for millimeter-wave applications. The detectors are fabricated on single-crystal silicon, which functions as a low-loss dielectric substrate for the microwave…

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

Pixelated silicon detectors are state-of-the-art technology to achieve precise tracking and vertexing at collider experiments, designed to accurately measure the hit position of incoming particles in high rate and radiation environments.…

Instrumentation and Detectors · Physics 2021-12-08 I. Zoi , A. Ebrahimi , F. Feindt , E. Garutti , P. Gunnellini , A. Hinzmann , C. Niemeyer , D. Pitzl , J. Schwandt , G. Steinbrück

Results of beam tests with planar silicon pixel sensors aimed towards the ATLAS Insertable B-Layer and High Luminosity LHC (HL-LHC) upgrades are presented. Measurements include spatial resolution, charge collection performance and charge…

Silicon trackers at the SLHC will suffer high radiation damage from particles produced during the collisions, which leads to high leakage currents. Reducing these currents in the sensors requires efficient cooling to -30 C. The large heat…

Instrumentation and Detectors · Physics 2008-11-19 Wim de Boer , Jochen Ebert

The reliability of bump connection structures has become a critical aspect of future silicon detectors for particle physics. The High Granularity Timing Detector (HGTD) for the ATLAS experiment at the High-Luminosity Large Hadron Collider…

Instrumentation and Detectors · Physics 2025-09-18 Y. Li , A. Aboulhorma , M. Ait Tamlihat , H. M. Alfanda , N. Atanov , O. Atanova , I. Azzouzi , J. Barreiro Guimarães Da Costa , T. Beau , D. Benchekroun , F. Bendebba , 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 , Y. Che , X. Chen , R. Cherkaoui El Moursli , E. Y. S. Chow , L. D. Corpe , C. G. Crozatier , L. D'Eramo , S. Dahbi , D. Dannheim , G. Daubard , Y. I. Davydov , C. de La Taille , J. Debevc , Y. Degerli , E. Delagnes , F. Deliot , M. Dhellot , G. Di Gregorio , P. Dinaucourt , P. J. Dos Santos De Assis , C. Duan , O. Duarte , F. Dulucq , J. Ehrecke , Y. El Ghazali , A. El Moussaouy , R. Estevam , A. Falou , L. Fan , Z. Fan , Y. Fan , K. Farman , F. Fassi , Y. Feng , M. Ferreira , F. Filthaut , F. Fischer , J. Fu , P. Fusté , G. Gaspar De Andrade , 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 , K. Hu , Y. Huang , X. Huang , C. Insa , J. Jeglot , X. Jia , G. Kramberger , M. Kuriyama , B. Y. Ky , D. Lacour , A. Lafarge , B. Lakssir , A. Lantheaume , D. Laporte , A. Leopold , M. Li , S. Li , L. Li , S. Li , H. Li , Z. Li , Z. Liang , S. Liang , M. A. Lisboa Leite , B. Liu , Y. L. Liu , K. Liu , K. Liu , Y. W. Liu , M. Lu , Y. J. Lu , F. L. Lucio Alves , F. Lyu , X. Ma , K. Ma , 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 , 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 , J. Pinol Bel , P. -O. Puhl , M. Puklavec , M. Qi , J. Qin , H. Ren , H. Riani , S. Ridaouni , V. Rogozin , L. Royer , F. Rudnyckyj , E. F. Saad , G. T. Saito , A. Salem , H. Santos , Ph. Schwemling , N. Seguin-Moreau , L. Serin , R. P. Serrano Fernandez , Q. Sha , A. Shaikovskii , 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 , J. Wan , W. Wang , C. Wang , Y. Wang , Y. Wang , A. Wang , T. Wang , T. Wang , S. M. Wang , Q. Weitzel , J. Wu , W. Wu , Y. Wu , M. Wu , L. Xia , H. Xu , D. Xu , L. Xu , Z. Yan , X. Yang , X. Yang , H. Yang , H. Yang , J. Ye , I. Youbi , J. Yuan , I. Zahir , H. Zeng , T. Zhang , J. Zhang , Z. Zhang , L. Zhang , D. Zhang , M. Zhao , Z. Zhao , X. Zheng , Z. Zhou , Y. Zhu , X. Zhuang

The ATLAS experiment, at the Large Hadron Collider, will incorporate discrete, high-resolution tracking sub-systems in the form of segmented silicon detectors with 40MHz radiation-hard readout electronics. In the region closest to the pp…

High Energy Physics - Experiment · Physics 2007-05-23 John Richardson , representing the ATLAS Pixel Project

The CMS tracker consists of two tracking systems utilizing semiconductor technology: the inner pixel and the outer strip detectors. The tracker detectors occupy the volume around the beam interaction region between 3 cm and 110 cm in radius…

Instrumentation and Detectors · Physics 2018-01-10 Viktor Veszpremi

In next ten years, the Large Hadron Collider will be upgraded to the High Luminosity LHC (HL-LHC), resulting in ten time more integrated luminosity. To withstand the much harsher radiation and occupancy conditions of the HL-LHC, the inner…

Instrumentation and Detectors · Physics 2019-05-01 Zhijun Liang

The CMS pixel detector has been designed for a peak luminosity of 10^34cm-2s-1 and a total dose corresponding to 2 years of LHC operation at a radius of 4 cm from the interaction region. Parts of the pixel detector will have to be replaced…

Instrumentation and Detectors · Physics 2010-01-25 H. C. Kästli

Applications such as augmented and virtual reality (AR/VR), optical atomic clocks, and quantum computing require photonic integration of (near-)visible laser sources to enable commercialization at scale. The heterogeneous integration of…

The LHC Phase-II upgrade will lead to a significant increase in luminosity, which in turn will bring new challenges for the operation of inner tracking detectors. A possible solution is to use active silicon sensors, taking advantage of…

Detectors at future $e^+e^-$ colliders need special calorimeters in the very forward region for a fast estimate and precise measurement of the luminosity, to improve the hermeticity and mask the central tracking detectors from backscattered…

High Energy Physics - Experiment · Physics 2023-01-24 Ivan Smiljanic

Results on beam tests of 3D silicon pixel sensors aimed at the ATLAS Insertable-B-Layer and High Luminosity LHC (HL-LHC)) upgrades are presented. Measurements include charge collection, tracking efficiency and charge sharing between pixel…

CLIC is a proposed linear e+e- collider designed to provide particle collisions at center-of-mass energies of up to 3 TeV. Precise measurements of the properties of the top quark and the Higgs boson, as well as searches for Beyond the…

Instrumentation and Detectors · Physics 2017-06-21 Simon Spannagel

CLIC is a proposed linear $e^{+}e^{-}$ collider with center-of-mass energies of up to $3\,\textrm{TeV}$. Its main objectives are precise top quark and Higgs boson measurements, as well as searches for Beyond Standard Model physics. To meet…

Instrumentation and Detectors · Physics 2018-12-07 Simon Spannagel

The High Luminosity Large Hadron Collider (HL-LHC) at CERN is expected to collide protons at a center-of-mass energy of 14 TeV and to reach the unprecedented peak instantaneous luminosity of $7.5 \times 10^{34} \text{cm}^{-2} \text{s}^{-1}$…

Instrumentation and Detectors · Physics 2023-01-26 Sascha Liechti

To cope with the harsh environment foreseen at the high luminosity conditions of HL- LHC, the ATLAS pixel detector has to be upgraded to be fully efficient with a good granularity, a maximized geometrical acceptance and an high read out…

The planned HL-LHC (High Luminosity LHC) in 2025 is being designed to maximise the physics potential through a sizable increase in the luminosity up to 6*10^34 cm^-2 s^-1. A consequence of this increased luminosity is the expected radiation…

The successful running of the large area Silicon trackers of ATLAS and CMS at LHC, and the ongoing R&D for the upgrade of these tracking systems, in various stages, over this decade, are a full proof of this technology and of its still…

Instrumentation and Detectors · Physics 2012-03-06 Aurore Savoy-Navarro