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CMS Phase-2 Inner Tracker Upgrade

The HL-LHC conditions of instantaneous peak luminosity up to 7.5x10$^{34}$ cm$^{-2}$ s$^{-1}$ and an integrated luminosity of the order of 300 fb$^{-1}$\slash year is expected to result in 1 MeV neutron equivalent fluence of 2.3 x 10$^{16}$ n$_{eq}$\slash cm$^{2}$ and a total ionizing dose (TID) of...

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Autor principal: Malik, Sudhir
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1742-6596/2374/1/012053
http://cds.cern.ch/record/2816244
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author Malik, Sudhir
author_facet Malik, Sudhir
author_sort Malik, Sudhir
collection CERN
description The HL-LHC conditions of instantaneous peak luminosity up to 7.5x10$^{34}$ cm$^{-2}$ s$^{-1}$ and an integrated luminosity of the order of 300 fb$^{-1}$\slash year is expected to result in 1 MeV neutron equivalent fluence of 2.3 x 10$^{16}$ n$_{eq}$\slash cm$^{2}$ and a total ionizing dose (TID) of 12 MGy (1.2 Grad) at the center of the CMS Experiment, where its innermost component, the Phase-2 Pixel Detector will be installed. This detector has to survive the above radiation dose, handle hit rates of 3.2 GHz\slash cm${^2}$ in the layers closest to the beam line, be able to track and separate particles in extremely dense collisions, deal with a pileup of 140-200 collisions per bunch crossing and have a high impact parameter resolution. This translates into a highly granular detector design with thinner sensors and smaller pixels, and a faster and more radiation hard electronics compared to the Phase-1 detector. This contribution reviews the Phase-2 upgrade of the (silicon-based) CMS Inner Tracker focusing on the features of the detector layout and on developments of pixelated devices.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2021
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spelling cern-28162442023-06-07T13:09:06Zdoi:10.1088/1742-6596/2374/1/012053http://cds.cern.ch/record/2816244engMalik, SudhirCMS Phase-2 Inner Tracker UpgradeDetectors and Experimental TechniquesThe HL-LHC conditions of instantaneous peak luminosity up to 7.5x10$^{34}$ cm$^{-2}$ s$^{-1}$ and an integrated luminosity of the order of 300 fb$^{-1}$\slash year is expected to result in 1 MeV neutron equivalent fluence of 2.3 x 10$^{16}$ n$_{eq}$\slash cm$^{2}$ and a total ionizing dose (TID) of 12 MGy (1.2 Grad) at the center of the CMS Experiment, where its innermost component, the Phase-2 Pixel Detector will be installed. This detector has to survive the above radiation dose, handle hit rates of 3.2 GHz\slash cm${^2}$ in the layers closest to the beam line, be able to track and separate particles in extremely dense collisions, deal with a pileup of 140-200 collisions per bunch crossing and have a high impact parameter resolution. This translates into a highly granular detector design with thinner sensors and smaller pixels, and a faster and more radiation hard electronics compared to the Phase-1 detector. This contribution reviews the Phase-2 upgrade of the (silicon-based) CMS Inner Tracker focusing on the features of the detector layout and on developments of pixelated devices.CMS-CR-2021-087oai:cds.cern.ch:28162442021-06-19
spellingShingle Detectors and Experimental Techniques
Malik, Sudhir
CMS Phase-2 Inner Tracker Upgrade
title CMS Phase-2 Inner Tracker Upgrade
title_full CMS Phase-2 Inner Tracker Upgrade
title_fullStr CMS Phase-2 Inner Tracker Upgrade
title_full_unstemmed CMS Phase-2 Inner Tracker Upgrade
title_short CMS Phase-2 Inner Tracker Upgrade
title_sort cms phase-2 inner tracker upgrade
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1088/1742-6596/2374/1/012053
http://cds.cern.ch/record/2816244
work_keys_str_mv AT maliksudhir cmsphase2innertrackerupgrade