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Related papers: The INFN-FBK Phase-2 R{\&}D Program

200 papers

The LHC accelerator complex will be upgraded between 2020-2022, to the High-Luminosity-LHC, to considerably increase statistics for the various physics analyses. To operate under these challenging new conditions, and maintain excellent…

Instrumentation and Detectors · Physics 2015-04-09 C. Nellist , N. Dinu , E. Gkougkousis , A. Lounis

The LHC machine is planning an upgrade program, which will smoothly bring the instantaneous luminosity to about $5-7.5\times10^{34}~\mathrm{cm}^{-2}\mathrm{s}^{-1}$ in 2028, to possibly reach an integrated luminosity of 3000-4500 fb$^{-1}$…

Instrumentation and Detectors · Physics 2019-11-07 Ernesto Migliore

The phase 1 upgrade of the CMS pixel detector has been designed to maintain the tracking performance at instantaneous luminosities of $2 \times 10^{34} \mathrm{~cm}^{-2} \mathrm{~s}^{-1}$. Both barrel and endcap disk systems now feature one…

Instrumentation and Detectors · Physics 2018-07-25 Jory Sonneveld

A wealth of physics results have already been obtained from the LHC, due to the excellent performance of the collider and its experiments. Even more results are expected to be achievable in the phase of the high-luminosity LHC (HL-LHC). It…

High Energy Physics - Experiment · Physics 2021-05-26 Susanne Kuehn

The ATLAS experiment pixel detector upgrade plans are focused on development of new technology, including the FE-I4 readout integrated circuit. The first upgrade project to make use of this new technology is an "Insertable B-Layer" (IBL)…

Instrumentation and Detectors · Physics 2011-09-23 M. Garcia-Sciveres , ATLAS Collaboration

For its physics program with a high-intensity hadron beam of up to 2e7 particles/s, the COMPASS experiment at CERN requires tracking of charged particles scattered by very small angles with respect to the incident beam direction. While good…

The CMS experiment at the LHC includes a hybrid silicon pixel detector for the reconstruction of charged tracks and of the interaction vertices. The detector is made of three barrel layers and two disks at each end of the barrel. Detector…

Instrumentation and Detectors · Physics 2007-10-29 Vincenzo Chiochia

We have developed two radiation-hard ASICs for optical data transmission in the ATLAS pixel detector at the LHC at CERN: a driver chip for a Vertical Cavity Surface Emitting Laser (VCSEL) diode for 80 Mbit/s data transmission from the…

A study of 3D pixel sensors of cell size 50 {\mu}m x 50 {\mu}m fabricated at IMB-CNM using double-sided n-on-p 3D technology is presented. Sensors were bump-bonded to the ROC4SENS readout chip. For the first time in such a small-pitch…

As photonic technologies continue to grow in multidimensional aspects, integrated photonics holds a unique position and continuously presents enormous possibilities to research communities. Applications span across data centers,…

A novel approach for designing the next generation of vertex detectors foresees to employ wafer-scale sensors that can be bent to truly cylindrical geometries after thinning them to thicknesses of 20-40$\mu$m. To solidify this concept, the…

Instrumentation and Detectors · Physics 2021-08-18 ALICE ITS project , : , G. Aglieri Rinella , M. Agnello , B. Alessandro , F. Agnese , R. S. Akram , J. Alme , E. Anderssen , D. Andreou , F. Antinori , N. Apadula , P. Atkinson , R. Baccomi , A. Badalà , A. Balbino , C. Bartels , R. Barthel , F. Baruffaldi , I. Belikov , S. Beole , P. Becht , A. Bhatti , M. Bhopal , N. Bianchi , M. B. Blidaru , G. Boca , J. Bok , G. Bonomi , M. Bonora , M. Borri , V. Borshchov , E. Botta , G. E. Bruno , M. Buckland , S. Bufalino , M. Cai , P. Camerini , P. Cariola , F. Catalano , C. Ceballos Sanchez , I. Chakaberia , M. Chartier , F. Colamaria , D. Colella , A. Collu , M. Concas , G. Contin , S. Costanza , P. Cui , A. Dainese , J. B. Dainton , L. De Cilladi , C. De Martin , G. De Robertis , W. Deng , A. Di Mauro , Y. Ding , M. Durkac , D. Elia , M. R. Ersdal , M. Faggin , F. Fan , A. Fantoni , P. Fecchio , A. Feliciello , G. Feofilov , A. Ferk , J. Ferencei , G. Fiorenza , A. N. Flores , E. Fragiacomo , D. Gajanana , A. Gal , C. Gao , C. Gargiulo , P. Gianotti , P. Giubilato , A. Grant , L. Greiner , A. Grelli , O. S. Groettvik , F. Grosa , C. Guo Hu , R. Hannigan , J. A. Hasenbichler , H. Helstrup , H. Hillemanns , C. Hills , P. Hindley , B. Hippolyte , B. Hofman , G. H. Hong , G. Huang , J. P. Iddon , H. Ilyas , M. A. Imhoff , A. Isakov , A. Jadlovska , S. Jadlovska , J. Jadlovsky , S. Jaelani , T. Johnson , A. Junique , P. Kalinak , A. Kalweit , M. Keil , Z. Khabanova , H. Khan , B. Kim , C. Kim , J. Kim , J. Kim , T. Kim , J. Klein , A. Kluge , C. Kobdaj , A. Kotliarov , I. Králik , F. Krizek , T. Kugathasan , C. Kuhn , P. G. Kuijer , S. Kushpil , M. J. Kweon , J. Y. Kwon , Y. Kwon , P. La Rocca , A. Lakrathok , R. Langoy , P. Larionov , E. Laudi , T. Lazareva , R. Lea , R. C. Lemmon , X. L. Li , J. Lien , B. Lim , S. H. Lim , S. Lindsay , A. Liu , J. Liu , J. Liu , M. Lunardon , G. Luparello , M. Lupi , M. Mager , A. Maire , Q. W. Malik , G. Mandaglio , V. Manzari , Y. Mao , G. V. Margagliotti , C. Markert , D. Marras , P. Martinengo , S. Masciocchi , M. Masera , A. Masoni , A. Mastroserio , P. F. T. Matuoka , G. Mazza , F. Mazzaschi , M. A. Mazzoni , F Morel , V. Muccifora , A. Mulliri , L. Musa , S. V. Nesbo , D. Nesterov , J. Norman , J. Park , R. N Patra , C. Pastore , H. Pei , X. Peng , S. Piano , C. Pinto , S. Pisano , S. Politano , E. Prakasa , F. Prino , M. Protsenko , M. Puccio , A. Rachevski , L. Ramello , F. Rami , I. Ravasenga , A. Rehman , F. Reidt , F. Riggi , K. Røed , D. Röhrich , F. Ronchetti , A. Rosano , M. J. Rossewij , A. Rossi , R. Rui , R. Russo , R. Sadikin , V. Sarritzu , J. Schambach , S. Senyukov , J. J. Seo , R. Shahoyan , S. Shaukat , S. Siddhanta , M. Sitta , R. J. M. Snellings , W. Snoeys , A. Songmoolnak , J. Sonneveld , F. Soramel , M. Suljic , S. Sumowidagdo , D. Sun , X. Sun , G. J. Tambave , G. Tersimonov , M. Tkacik , M. Toppi , A. Trifiró , S. Trogolo , V. Trubnikov , R. Turrisi , T. S. Tveter , I. Tymchuck , K. Ullaland , M. Urioni , G. L. Usai , N. Valle , L. V. R. van Doremalen , T. Vanat , J. W. Van Hoorne , M. Varga-Kofarago , A. Velure , D. Wang , Y. Wang , J. Wikne , J. R. Wright , R. Xu , P. Yang , Z. Yin , I. -K. Yoo , J. H. Yoon , S. Yuan , V. Zaccolo , E. Zhang , X. Zhang , V. Zherebchevskii , D. Zhou , J. Zhu , Y. Zhu , G. Zinovjev , N. Zurlo

To fully exploit the increased luminosity of the HL-LHC, the CMS Inner Tracker is undergoing a major upgrade to withstand extreme radiation levels and data rates, while improving granularity and reducing material budget. The upgraded…

Instrumentation and Detectors · Physics 2025-06-12 Panagiotis Assiouras

The ATLAS Forward Proton (AFP) detector is intended to measure protons scattered at small angles from the ATLAS interaction point. To this end, a combination of 3D Silicon pixel tracking modules and Quartz-Cherenkov time-of-flight (ToF)…

The Insertable B-layer (IBL) is a fourth pixel layer that will be added inside the existing ATLAS pixel detector during the long LHC shutdown of 2013 and 2014. The new four layer pixel system will ensure excellent tracking, vertexing and…

Instrumentation and Detectors · Physics 2013-04-17 Malte Backhaus

The ATLAS Insertable B-Layer (IBL) is the innermost layer of pixel detectors, and was installed in May 2014 at a radius of 3.3 cm from the beam axis, between the existing Pixel detector and a new smaller radius beam-pipe. The new detector,…

Instrumentation and Detectors · Physics 2017-01-16 Alessandro La Rosa

A new pixel detector for the CMS experiment is being built, owing to the instantaneous luminosities anticipated for the Phase I Upgrade of the LHC. The new CMS pixel detector provides four-hit tracking while featuring a significantly…

Instrumentation and Detectors · Physics 2016-12-23 Simon Spannagel

The upgraded Inner Tracking System (ITS2) of the ALICE experiment at the CERN Large Hadron Collider is based on Monolithic Active Pixel Sensors (MAPS). With a sensitive area of about 10 $m^2$ and 12.5 billion pixels, ITS2 represents the…

Instrumentation and Detectors · Physics 2025-05-29 Nicolo' Valle

Monolithic Active Pixel Sensors (MAPS) achieved widespread use in several scientific applications, thanks to their properties, such as low material budget and high granularity. The ARCADIA INFN project developed a Fully-Depleted MAPS…

Hybrid pixel detectors have been invented for the LHC to make tracking and vertexing possible at all in LHC's radiation intense environment. The LHC pixel detectors have meanwhile very successfully fulfilled their promises and R\&D for the…

Instrumentation and Detectors · Physics 2016-01-06 Norbert Wermes

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