Measurements of time resolution of the RD50-MPW2 DMAPS prototype using TCT and $^{90}\mathrm{Sr}
Results in this paper present an in-depth study of time resolution for active pixels of the RD50-MPW2 prototype CMOS particle detector. Measurement techniques employed include Backside- and Edge-TCT configurations, in addition to electrons from a $^{90}\mathrm{Sr}$ source. A sample irradiated to $5\...
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creator | Debevc, J Franks, M Hiti, B Kraemer, U Kramberger, G Mandić, I Marco-Hernández, R Nobels, D. J. L Powell, S Sonneveld, J Steininger, H Tsolanta, C Vilella, E Zhang, C |
description | Results in this paper present an in-depth study of time resolution for active
pixels of the RD50-MPW2 prototype CMOS particle detector. Measurement
techniques employed include Backside- and Edge-TCT configurations, in addition
to electrons from a $^{90}\mathrm{Sr}$ source. A sample irradiated to $5\cdot
10^{14}\,\mathrm{n}_\mathrm{eq}/\mathrm{cm}^2$ was used to study the effect of
radiation damage. Timing performance was evaluated for the entire pixel matrix
and with positional sensitivity within individual pixels as a function of the
deposited charge. Time resolution obtained with TCT is seen to be uniform
throughout the pixel's central region with approx. $220\,\mathrm{ps}$ at
$12\,\mathrm{ke}^-$ of deposited charge, degrading at the edges and lower
values of deposited charge. $^{90}\mathrm{Sr}$ measurements show a slightly
worse time resolution as a result of delayed events coming from the peripheral
areas of the pixel. |
doi_str_mv | 10.48550/arxiv.2312.01793 |
format | Article |
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pixels of the RD50-MPW2 prototype CMOS particle detector. Measurement
techniques employed include Backside- and Edge-TCT configurations, in addition
to electrons from a $^{90}\mathrm{Sr}$ source. A sample irradiated to $5\cdot
10^{14}\,\mathrm{n}_\mathrm{eq}/\mathrm{cm}^2$ was used to study the effect of
radiation damage. Timing performance was evaluated for the entire pixel matrix
and with positional sensitivity within individual pixels as a function of the
deposited charge. Time resolution obtained with TCT is seen to be uniform
throughout the pixel's central region with approx. $220\,\mathrm{ps}$ at
$12\,\mathrm{ke}^-$ of deposited charge, degrading at the edges and lower
values of deposited charge. $^{90}\mathrm{Sr}$ measurements show a slightly
worse time resolution as a result of delayed events coming from the peripheral
areas of the pixel.</description><identifier>DOI: 10.48550/arxiv.2312.01793</identifier><language>eng</language><subject>Physics - Instrumentation and Detectors</subject><creationdate>2023-12</creationdate><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2312.01793$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2312.01793$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1088/1748-0221/19/05/P05068$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Debevc, J</creatorcontrib><creatorcontrib>Franks, M</creatorcontrib><creatorcontrib>Hiti, B</creatorcontrib><creatorcontrib>Kraemer, U</creatorcontrib><creatorcontrib>Kramberger, G</creatorcontrib><creatorcontrib>Mandić, I</creatorcontrib><creatorcontrib>Marco-Hernández, R</creatorcontrib><creatorcontrib>Nobels, D. J. L</creatorcontrib><creatorcontrib>Powell, S</creatorcontrib><creatorcontrib>Sonneveld, J</creatorcontrib><creatorcontrib>Steininger, H</creatorcontrib><creatorcontrib>Tsolanta, C</creatorcontrib><creatorcontrib>Vilella, E</creatorcontrib><creatorcontrib>Zhang, C</creatorcontrib><title>Measurements of time resolution of the RD50-MPW2 DMAPS prototype using TCT and $^{90}\mathrm{Sr}</title><description>Results in this paper present an in-depth study of time resolution for active
pixels of the RD50-MPW2 prototype CMOS particle detector. Measurement
techniques employed include Backside- and Edge-TCT configurations, in addition
to electrons from a $^{90}\mathrm{Sr}$ source. A sample irradiated to $5\cdot
10^{14}\,\mathrm{n}_\mathrm{eq}/\mathrm{cm}^2$ was used to study the effect of
radiation damage. Timing performance was evaluated for the entire pixel matrix
and with positional sensitivity within individual pixels as a function of the
deposited charge. Time resolution obtained with TCT is seen to be uniform
throughout the pixel's central region with approx. $220\,\mathrm{ps}$ at
$12\,\mathrm{ke}^-$ of deposited charge, degrading at the edges and lower
values of deposited charge. $^{90}\mathrm{Sr}$ measurements show a slightly
worse time resolution as a result of delayed events coming from the peripheral
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pixels of the RD50-MPW2 prototype CMOS particle detector. Measurement
techniques employed include Backside- and Edge-TCT configurations, in addition
to electrons from a $^{90}\mathrm{Sr}$ source. A sample irradiated to $5\cdot
10^{14}\,\mathrm{n}_\mathrm{eq}/\mathrm{cm}^2$ was used to study the effect of
radiation damage. Timing performance was evaluated for the entire pixel matrix
and with positional sensitivity within individual pixels as a function of the
deposited charge. Time resolution obtained with TCT is seen to be uniform
throughout the pixel's central region with approx. $220\,\mathrm{ps}$ at
$12\,\mathrm{ke}^-$ of deposited charge, degrading at the edges and lower
values of deposited charge. $^{90}\mathrm{Sr}$ measurements show a slightly
worse time resolution as a result of delayed events coming from the peripheral
areas of the pixel.</abstract><doi>10.48550/arxiv.2312.01793</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - Instrumentation and Detectors |
title | Measurements of time resolution of the RD50-MPW2 DMAPS prototype using TCT and $^{90}\mathrm{Sr} |
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