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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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Autor principal: Barberis, D
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0168-9002(00)00041-3
http://cds.cern.ch/record/446338
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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