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Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter

Intrinsic performance of the ATLAS calorimeters in the barrel region with respect to charged pions was studied. For this the following simulated data were used: pion energy scans ($E = 20, 50, 200, 400$ and $1000$ GeV) at two pseudo-rapidity points ($eta = 0.3$ and $1.3$) and pseudo-rapidity scans (...

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Detalles Bibliográficos
Autores principales: Bosman, M., Kulchitsky, Y., Nessi, M.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:http://cds.cern.ch/record/683874
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author Bosman, M.
Kulchitsky, Y.
Nessi, M.
author_facet Bosman, M.
Kulchitsky, Y.
Nessi, M.
author_sort Bosman, M.
collection CERN
description Intrinsic performance of the ATLAS calorimeters in the barrel region with respect to charged pions was studied. For this the following simulated data were used: pion energy scans ($E = 20, 50, 200, 400$ and $1000$ GeV) at two pseudo-rapidity points ($eta = 0.3$ and $1.3$) and pseudo-rapidity scans ($-0.2 < eta < 1.8$) with pions of constant transverse energy ($E_T = 20$ and $50$ GeV). For pion energy reconstruction the benchmark approach was used. Performance was estimated for cases, when energy and rapidity dependent and independent calibration parameters were applied. The best results were obtained with energy and rapidity dependent parameters. Studies done for pions enabled optimization of the cone size and of the cut to obtain the best energy resolution. Energy dependence of the resolution can be parameterized as: $(50pm4)%/sqrt{E} oplus (3.4pm0.3)% oplus 1.0/E$ at $eta = 0.3$ and $(68pm8)%/sqrt{E} oplus (3.0pm0.7)% oplus 1.5/E$ at $eta = 1.3$. Larger constant term at $eta=0.3$ can be explained by longitudinal leakage from calorimeters in this region. Resulted deviation from linearity in response is within $pm0.5$%. Resolution, obtained for pseudo-rapidity scans, can be described as: $(39pm1)%/sqrt{E} oplus (1pm5)%$ for $E_T = 20$ GeV and $(49pm9)%/sqrt{E} oplus (2pm6)%$ for $E_T = 50$ GeV, everywhere, except region around $eta = 1.5$, where resolution is spoiled by significant energy losses in dead materials. Distributions of response ($sigma/E_{beam}$) have 2.2% (1.1%) for $E_T = 20$ GeV ($50$ GeV). Analysis of tails of energy distribution was also presented.
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language eng
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spelling cern-6838742023-03-14T18:56:53Zhttp://cds.cern.ch/record/683874engBosman, M.Kulchitsky, Y.Nessi, M.Charged Pion Energy Reconstruction in the ATLAS Barrel CalorimeterDetectors and Experimental TechniquesIntrinsic performance of the ATLAS calorimeters in the barrel region with respect to charged pions was studied. For this the following simulated data were used: pion energy scans ($E = 20, 50, 200, 400$ and $1000$ GeV) at two pseudo-rapidity points ($eta = 0.3$ and $1.3$) and pseudo-rapidity scans ($-0.2 < eta < 1.8$) with pions of constant transverse energy ($E_T = 20$ and $50$ GeV). For pion energy reconstruction the benchmark approach was used. Performance was estimated for cases, when energy and rapidity dependent and independent calibration parameters were applied. The best results were obtained with energy and rapidity dependent parameters. Studies done for pions enabled optimization of the cone size and of the cut to obtain the best energy resolution. Energy dependence of the resolution can be parameterized as: $(50pm4)%/sqrt{E} oplus (3.4pm0.3)% oplus 1.0/E$ at $eta = 0.3$ and $(68pm8)%/sqrt{E} oplus (3.0pm0.7)% oplus 1.5/E$ at $eta = 1.3$. Larger constant term at $eta=0.3$ can be explained by longitudinal leakage from calorimeters in this region. Resulted deviation from linearity in response is within $pm0.5$%. Resolution, obtained for pseudo-rapidity scans, can be described as: $(39pm1)%/sqrt{E} oplus (1pm5)%$ for $E_T = 20$ GeV and $(49pm9)%/sqrt{E} oplus (2pm6)%$ for $E_T = 50$ GeV, everywhere, except region around $eta = 1.5$, where resolution is spoiled by significant energy losses in dead materials. Distributions of response ($sigma/E_{beam}$) have 2.2% (1.1%) for $E_T = 20$ GeV ($50$ GeV). Analysis of tails of energy distribution was also presented.The intrinsic performance of the ATLAS barrel and extended barrel calorimeters for the measurement of charged pions is presented. Pion energy scans (E = 20, 50, 200, 400 and 1000 GeV) at two pseudo-rapidity points ($\eta$ = 0.3 and 1.3) and pseudorapidity scans ($-0.2 < \eta < 1.8$) with pions of constant transverse energy ($E_T = 20$ and 50 GeV) are analysed. A simple approach, that accounts in first order for non-compensation and dead material effects, is used for the pion energy reconstruction. The intrinsic performances of the calorimeter are studied: resolution, linearity, effect of dead material, tails in the energy distribution. The effect of electronic noise, cell energy cuts and restricted cone size are investigated.hep-ex/0002033JINR-E1-2000-31oai:cds.cern.ch:6838741999
spellingShingle Detectors and Experimental Techniques
Bosman, M.
Kulchitsky, Y.
Nessi, M.
Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter
title Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter
title_full Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter
title_fullStr Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter
title_full_unstemmed Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter
title_short Charged Pion Energy Reconstruction in the ATLAS Barrel Calorimeter
title_sort charged pion energy reconstruction in the atlas barrel calorimeter
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/683874
work_keys_str_mv AT bosmanm chargedpionenergyreconstructionintheatlasbarrelcalorimeter
AT kulchitskyy chargedpionenergyreconstructionintheatlasbarrelcalorimeter
AT nessim chargedpionenergyreconstructionintheatlasbarrelcalorimeter