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Comparison of PET sensitivity with various scintillation crystals

https://repo.qst.go.jp/records/76864
https://repo.qst.go.jp/records/76864
424c2f6d-1df9-4fcf-a345-8fba4b173700
Item type 会議発表用資料 / Presentation(1)
公開日 2019-09-19
タイトル
タイトル Comparison of PET sensitivity with various scintillation crystals
言語
言語 eng
資源タイプ
資源タイプ識別子 http://purl.org/coar/resource_type/c_c94f
資源タイプ conference object
アクセス権
アクセス権 metadata only access
アクセス権URI http://purl.org/coar/access_right/c_14cb
著者 Kang, Hangyu

× Kang, Hangyu

WEKO 785042

Kang, Hangyu

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Nishikido, Fumihiko

× Nishikido, Fumihiko

WEKO 785043

Nishikido, Fumihiko

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Tashima, Hideaki

× Tashima, Hideaki

WEKO 785044

Tashima, Hideaki

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Yamaya, Taiga

× Yamaya, Taiga

WEKO 785045

Yamaya, Taiga

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Kang, Hangyu

× Kang, Hangyu

WEKO 785046

en Kang, Hangyu

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Nishikido, Fumihiko

× Nishikido, Fumihiko

WEKO 785047

en Nishikido, Fumihiko

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Tashima, Hideaki

× Tashima, Hideaki

WEKO 785048

en Tashima, Hideaki

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Yamaya, Taiga

× Yamaya, Taiga

WEKO 785049

en Yamaya, Taiga

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抄録
内容記述タイプ Abstract
内容記述 Positron emission tomography (PET) has been evolved with the development of new scintillation crystals such as LYSO and GAGG. The performance of a PET scanner is mainly determined by the characteristics of a scintillation crystal. The aim of this study is to compare the PET sensitivity with various scintillation crystals. In this study, a SIEMENS small animal Inveon PET (inner diameter= 161 mm, axial length= 127 mm) was modeled by using GATE Monte Carlo software (Fig.1). The Inveon PET scanner consists of 4 rings each of which has 16 detectors/ring. The PET detector block consists of 20×20 crystal array each of which has a dimension of 1.5×1.5×10 mm3. An F-18 point source with 1 MBq was placed at the center of the PET FOV and the simulation was performed for 1 s. The simulation was performed with various crystals such as BGO (Zeff=71, ρ=7.13 g/cm3), LSO (Zeff=65, ρ=7.4 g/cm3), LYSO (Zeff=61, ρ=7.20 g/cm3), GSO (Zeff=57, ρ=6.7 g/cm3), GAGG (Zeff=53, ρ=6.63 g/cm3), CsI (Zeff=54, ρ=4.51 g/cm3), and NaI (Zeff=50, ρ=3.67 g/cm3), respectively. The simulated sensitivities of BGO, LSO, LYSO, GAGG, and GSO were 12.44, 9.75, 8.61, 6.15, and 6.03%, respectively (Fig. 1(a)). The BGO resulted in a highest sensitivity and photo-fraction (Fig. 1(b)). The sensitivity of GAGG was 52% lower than that of BGO crystal. In future, the simulation results will be validated by experimental measurements.
会議概要(会議名, 開催地, 会期, 主催者等)
内容記述タイプ Other
内容記述 15th Int. SCINT 2019
発表年月日
日付 2019-10-01
日付タイプ Issued
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