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  • To avoid inefficiency and inhomogeneity of BSE scintillation detection systems, efficient transport of photons from luminescent centres in a scintillator to a photocathode of a photomultiplier tube must be provided. Optimization of the photon transport of a rotationally symmetric Everhart-Thornley detector is quite a feasible task, because a code for the Monte Carlo (MC) simulation is based on the system geometry which is a function of one variable coordinate. For such a rotationally symmetric detection system the previous MC code Scintil was developed in our laboratory. The Scintil code includes photon generation in a point source, mirror reflection by a metal coated surface, Fresnel reflection by a metal uncoated surface, Fresnel passage through the boundary of different materials, diffusion reflection and passage through a matted surface and optical absorption in material.
  • To avoid inefficiency and inhomogeneity of BSE scintillation detection systems, efficient transport of photons from luminescent centres in a scintillator to a photocathode of a photomultiplier tube must be provided. Optimization of the photon transport of a rotationally symmetric Everhart-Thornley detector is quite a feasible task, because a code for the Monte Carlo (MC) simulation is based on the system geometry which is a function of one variable coordinate. For such a rotationally symmetric detection system the previous MC code Scintil was developed in our laboratory. The Scintil code includes photon generation in a point source, mirror reflection by a metal coated surface, Fresnel reflection by a metal uncoated surface, Fresnel passage through the boundary of different materials, diffusion reflection and passage through a matted surface and optical absorption in material. (en)
  • K zamezení neúčinných a nehomogenních BSE scintilačních detekčních systémů musí být zajištěn účinný transport fotonů z luminiscenčních center ve scintilátoru k fotokatodě fotoelektrického násobiče. Optimalizace transportu fotonů v rotačně symetrických Everhart-Thornley detektorech je dost schůdný úkol, protože kód pro Monte Carlo (MC) simulaci je založen na geometrii systému, která je funkcí jedné proměnné souřadnice. Pro takový rotačně symetrický detekční systém byl v naší laboratoři vyvinut předešlý MC kód Scintil. Kód Scintil zahrnuje vznik fotonu v bodovém zdroji, zrcadlový odraz na kovem pokrytém povrchu, Fresnelův odraz na kovem nepokrytém povrchu, Fresnelův průchod rozhraním různých materiálů, difúzní odraz na a průchod přes matovaný povrch a optickou absorpci v materiálu. (cs)
Title
  • Extended Algorithm for Optimization of Photon Transport in Scintillation Detector
  • Extended Algorithm for Optimization of Photon Transport in Scintillation Detector (en)
  • Rozšířený algoritmus pro optimalizaci transportu fotonů ve scintilačním Detektoru (cs)
skos:prefLabel
  • Extended Algorithm for Optimization of Photon Transport in Scintillation Detector
  • Extended Algorithm for Optimization of Photon Transport in Scintillation Detector (en)
  • Rozšířený algoritmus pro optimalizaci transportu fotonů ve scintilačním Detektoru (cs)
skos:notation
  • RIV/68081731:_____/05:00022406!RIV06-GA0-68081731
http://linked.open.../vavai/riv/strany
  • 55
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  • P(GA102/04/2144)
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  • 521238
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  • RIV/68081731:_____/05:00022406
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  • scintillation detector; photon transport; Monte Carlo simulation (en)
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  • [D1BAC7C9C4E6]
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  • Davos
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  • Proceedings - Microscopy Conference 2005 - Dreiländertagung /6./
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  • Autrata, Rudolf
  • Schauer, Petr
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issn
  • 1019-6447
number of pages
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  • Paul Scherrer Institute
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