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ATLAS Inner Detector developments
The ATLAS Inner Detector consists of three layers of silicon pixels, four double layers of silicon microstrips and a Transition Radiation Tracker (straw tubes). The good performance of the track and vertex reconstruction algorithms is a direct consequence of the small radius (4.3, 10.1 and 13.2 cm),...
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Lenguaje: | eng |
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1999
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Acceso en línea: | https://dx.doi.org/10.1016/S0168-9002(00)00041-3 http://cds.cern.ch/record/446338 |
_version_ | 1780895964983197696 |
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author | Barberis, D |
author_facet | Barberis, D |
author_sort | Barberis, D |
collection | CERN |
description | The ATLAS Inner Detector consists of three layers of silicon pixels, four double layers of silicon microstrips and a Transition Radiation Tracker (straw tubes). The good performance of the track and vertex reconstruction algorithms is a direct consequence of the small radius (4.3, 10.1 and 13.2 cm), fine pitch ($50 \times 300~\mu$m) and low occupancy ($<3 \times 10^{-4}$ at design luminosity) of the pixel detectors, and of the good tracking capabilities of the SCT and the TRT. The full detector simulation is used to evaluate the performance of the detector and of the reconstruction algorithms. Results are presented on track and vertex reconstruction efficiencies and resolutions, and on the separation between $b$-jets and jets produced by light quarks. |
id | cern-446338 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1999 |
record_format | invenio |
spelling | cern-4463382019-09-30T06:29:59Zdoi:10.1016/S0168-9002(00)00041-3http://cds.cern.ch/record/446338engBarberis, DATLAS Inner Detector developmentsDetectors and Experimental TechniquesThe ATLAS Inner Detector consists of three layers of silicon pixels, four double layers of silicon microstrips and a Transition Radiation Tracker (straw tubes). The good performance of the track and vertex reconstruction algorithms is a direct consequence of the small radius (4.3, 10.1 and 13.2 cm), fine pitch ($50 \times 300~\mu$m) and low occupancy ($<3 \times 10^{-4}$ at design luminosity) of the pixel detectors, and of the good tracking capabilities of the SCT and the TRT. The full detector simulation is used to evaluate the performance of the detector and of the reconstruction algorithms. Results are presented on track and vertex reconstruction efficiencies and resolutions, and on the separation between $b$-jets and jets produced by light quarks.ATL-CONF-99-003oai:cds.cern.ch:4463381999-09-01 |
spellingShingle | Detectors and Experimental Techniques Barberis, D ATLAS Inner Detector developments |
title | ATLAS Inner Detector developments |
title_full | ATLAS Inner Detector developments |
title_fullStr | ATLAS Inner Detector developments |
title_full_unstemmed | ATLAS Inner Detector developments |
title_short | ATLAS Inner Detector developments |
title_sort | atlas inner detector developments |
topic | Detectors and Experimental Techniques |
url | https://dx.doi.org/10.1016/S0168-9002(00)00041-3 http://cds.cern.ch/record/446338 |
work_keys_str_mv | AT barberisd atlasinnerdetectordevelopments |