Cargando…

The ATLAS High Granularity Timing Detector

The addition of The High Granularity Timing Detector (HGTD) in ATLAS offers to solve many challenges that are faced in the High Luminosity LHC (HI LHC) Conditions. It covers the forward region of 2.4 < |η | < 4.0, and decreases the effects of the pile-up. The sensors′ choice are the Low Gain Ava...

Descripción completa

Detalles Bibliográficos
Autor principal: Al Shamsi, Maitha Ahmed
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:http://cds.cern.ch/record/2651090
_version_ 1780960848033873920
author Al Shamsi, Maitha Ahmed
author_facet Al Shamsi, Maitha Ahmed
author_sort Al Shamsi, Maitha Ahmed
collection CERN
description The addition of The High Granularity Timing Detector (HGTD) in ATLAS offers to solve many challenges that are faced in the High Luminosity LHC (HI LHC) Conditions. It covers the forward region of 2.4 < |η | < 4.0, and decreases the effects of the pile-up. The sensors′ choice are the Low Gain Avalanche Detector (LGAD). The results that are presented in this paper are obtained from test beams in June 2018 with a pion beam. The two chosen LGAD sensors are W9LGA35 and BNL W1835 from batch 1xx, their characteristics (e.g charge and amplitude distributions) were investigated from a reference (SiPM) in order to study their performance and measure the time resolution using Constant Fraction Discriminator (CFD) method. Both sensors were performing poorly due to a technical issue in the reference. However, W9LGA35′s performance was showing better results.
id cern-2651090
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
record_format invenio
spelling cern-26510902019-09-30T06:29:59Zhttp://cds.cern.ch/record/2651090engAl Shamsi, Maitha AhmedThe ATLAS High Granularity Timing DetectorPhysics in GeneralThe addition of The High Granularity Timing Detector (HGTD) in ATLAS offers to solve many challenges that are faced in the High Luminosity LHC (HI LHC) Conditions. It covers the forward region of 2.4 < |η | < 4.0, and decreases the effects of the pile-up. The sensors′ choice are the Low Gain Avalanche Detector (LGAD). The results that are presented in this paper are obtained from test beams in June 2018 with a pion beam. The two chosen LGAD sensors are W9LGA35 and BNL W1835 from batch 1xx, their characteristics (e.g charge and amplitude distributions) were investigated from a reference (SiPM) in order to study their performance and measure the time resolution using Constant Fraction Discriminator (CFD) method. Both sensors were performing poorly due to a technical issue in the reference. However, W9LGA35′s performance was showing better results.CERN-STUDENTS-Note-2018-223oai:cds.cern.ch:26510902018-12-13
spellingShingle Physics in General
Al Shamsi, Maitha Ahmed
The ATLAS High Granularity Timing Detector
title The ATLAS High Granularity Timing Detector
title_full The ATLAS High Granularity Timing Detector
title_fullStr The ATLAS High Granularity Timing Detector
title_full_unstemmed The ATLAS High Granularity Timing Detector
title_short The ATLAS High Granularity Timing Detector
title_sort atlas high granularity timing detector
topic Physics in General
url http://cds.cern.ch/record/2651090
work_keys_str_mv AT alshamsimaithaahmed theatlashighgranularitytimingdetector
AT alshamsimaithaahmed atlashighgranularitytimingdetector