000891110 001__ 891110
000891110 005__ 20250129092455.0
000891110 0247_ $$2doi$$a10.1109/TNS.2021.3049675
000891110 0247_ $$2ISSN$$a0018-9499
000891110 0247_ $$2ISSN$$a1558-1578
000891110 0247_ $$2Handle$$a2128/28686
000891110 0247_ $$2WOS$$aWOS:000631201300011
000891110 037__ $$aFZJ-2021-01371
000891110 041__ $$aEnglish
000891110 082__ $$a620
000891110 1001_ $$0P:(DE-Juel1)169828$$aKumar, S.$$b0$$eCorresponding author
000891110 245__ $$aNonlinearity Simulation of Digital SiPM Response for Inhomogeneous Light
000891110 260__ $$aNew York, NY$$bIEEE$$c2021
000891110 3367_ $$2DRIVER$$aarticle
000891110 3367_ $$2DataCite$$aOutput Types/Journal article
000891110 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1632383978_767
000891110 3367_ $$2BibTeX$$aARTICLE
000891110 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000891110 3367_ $$00$$2EndNote$$aJournal Article
000891110 520__ $$aCurrently we are developing a neutron scintillationdetector prototype using silicon photomultipliers (SiPM) as thephotodetector. In order to reconstruct the position of single neutronevents to a better accuracy than the pixel pitch of the SiPM,a very accurate photon count is required. Each pixel consistsof 3200 micro-cells, operated in Geiger mode. A cell which isalready triggered cannot detect any following photons hittingthe cell, until it is recharged. This leads to a non-linearity in thepixel’s response for a higher photon density impinging across the pixel. Previous studies provided a correction factor to estimatethe saturation, by assuming a homogeneous photon distributiondensity and comparing it to the number of micro-cells. In ourspecific application, the photon distribution is not homogeneous,which is why we examined the influence of the homogeneity onthe saturation. In this work, we present a case study for differencein non-linearity effect for an in-homogeneous and homogeneousphoton distribution density, given the light intensity is equal.The simulation results suggest that the effect could be higher foran in-homogeneous distribution. Therefore, care must be takenwhen using the established correction factor for saturation andan analysis of the photon distribution homogeneity is necessary.
000891110 536__ $$0G:(DE-HGF)POF4-2171$$a2171 - Biological and environmental resources for sustainable use (POF4-217)$$cPOF4-217$$fPOF IV$$x0
000891110 588__ $$aDataset connected to CrossRef
000891110 65027 $$0V:(DE-MLZ)SciArea-220$$2V:(DE-HGF)$$aInstrument and Method Development$$x0
000891110 65017 $$0V:(DE-MLZ)GC-1601-2016$$2V:(DE-HGF)$$aEngineering, Industrial Materials and Processing$$x0
000891110 693__ $$0EXP:(DE-MLZ)TREFF-20140101$$1EXP:(DE-MLZ)FRMII-20140101$$5EXP:(DE-MLZ)TREFF-20140101$$6EXP:(DE-MLZ)NL5S-20140101$$aForschungs-Neutronenquelle Heinz Maier-Leibnitz $$eTREFF: Neutronenreflektometer$$fNL5S$$x0
000891110 7001_ $$0P:(DE-Juel1)156322$$aHerzkamp, Matthias$$b1
000891110 7001_ $$0P:(DE-Juel1)142562$$avan Waasen, S.$$b2
000891110 773__ $$0PERI:(DE-600)2025398-9$$a10.1109/TNS.2021.3049675$$gVol. 68, no. 3, p. 354 - 358$$n3$$p354 - 358$$tIEEE transactions on nuclear science$$v68$$x1558-1578$$y2021
000891110 8564_ $$uhttps://juser.fz-juelich.de/record/891110/files/Nonlinearity_Simulation_of_Digital_SiPM_Response_for_Inhomogeneous_Light.pdf
000891110 8564_ $$uhttps://juser.fz-juelich.de/record/891110/files/FINAL%20VERSION.pdf$$yOpenAccess
000891110 909CO $$ooai:juser.fz-juelich.de:891110$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000891110 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)169828$$aForschungszentrum Jülich$$b0$$kFZJ
000891110 9101_ $$0I:(DE-HGF)0$$6P:(DE-Juel1)156322$$aExternal Institute$$b1$$kExtern
000891110 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)142562$$aForschungszentrum Jülich$$b2$$kFZJ
000891110 9131_ $$0G:(DE-HGF)POF4-217$$1G:(DE-HGF)POF4-210$$2G:(DE-HGF)POF4-200$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF4-2171$$aDE-HGF$$bForschungsbereich Erde und Umwelt$$lErde im Wandel – Unsere Zukunft nachhaltig gestalten$$vFür eine nachhaltige Bio-Ökonomie – von Ressourcen zu Produkten$$x0
000891110 9130_ $$0G:(DE-HGF)POF3-899$$1G:(DE-HGF)POF3-890$$2G:(DE-HGF)POF3-800$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bProgrammungebundene Forschung$$lohne Programm$$vohne Topic$$x0
000891110 9141_ $$y2021
000891110 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0160$$2StatID$$aDBCoverage$$bEssential Science Indicators$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)1160$$2StatID$$aDBCoverage$$bCurrent Contents - Engineering, Computing and Technology$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bIEEE T NUCL SCI : 2019$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0113$$2StatID$$aWoS$$bScience Citation Index Expanded$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000891110 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline$$d2021-01-28
000891110 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2021-01-28
000891110 920__ $$lyes
000891110 9201_ $$0I:(DE-Juel1)ZEA-2-20090406$$kZEA-2$$lZentralinstitut für Elektronik$$x0
000891110 9801_ $$aFullTexts
000891110 980__ $$ajournal
000891110 980__ $$aVDB
000891110 980__ $$aUNRESTRICTED
000891110 980__ $$aI:(DE-Juel1)ZEA-2-20090406
000891110 981__ $$aI:(DE-Juel1)PGI-4-20110106