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A comparative study of PET images among different PET scanners for detection infinitesimal radioactivity

https://repo.qst.go.jp/records/70278
https://repo.qst.go.jp/records/70278
b74fa491-f680-4f67-aeea-5e67565ab869
Item type 会議発表用資料 / Presentation(1)
公開日 2010-10-19
タイトル
タイトル A comparative study of PET images among different PET scanners for detection infinitesimal radioactivity
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 Shiraishi, Takahiro

× Shiraishi, Takahiro

WEKO 690003

Shiraishi, Takahiro

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Yoshikawa, Kyosan

× Yoshikawa, Kyosan

WEKO 690004

Yoshikawa, Kyosan

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Tanimoto, Katsuyuki

× Tanimoto, Katsuyuki

WEKO 690005

Tanimoto, Katsuyuki

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Kuroiwa, Toshitaka

× Kuroiwa, Toshitaka

WEKO 690006

Kuroiwa, Toshitaka

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Ishii, Noriyuki

× Ishii, Noriyuki

WEKO 690007

Ishii, Noriyuki

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Yoshida, Eiji

× Yoshida, Eiji

WEKO 690008

Yoshida, Eiji

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Yamaya, Taiga

× Yamaya, Taiga

WEKO 690009

Yamaya, Taiga

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Murayama, Hideo

× Murayama, Hideo

WEKO 690010

Murayama, Hideo

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Ohashi, Seiya

× Ohashi, Seiya

WEKO 690011

Ohashi, Seiya

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Toubaru, Sachiko

× Toubaru, Sachiko

WEKO 690012

Toubaru, Sachiko

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Mizoe, Junetsu

× Mizoe, Junetsu

WEKO 690013

Mizoe, Junetsu

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Kamada, Tadashi

× Kamada, Tadashi

WEKO 690014

Kamada, Tadashi

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Watanabe, Kazuhiro

× Watanabe, Kazuhiro

WEKO 690015

Watanabe, Kazuhiro

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白石 貴博

× 白石 貴博

WEKO 690016

en 白石 貴博

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吉川 京燦

× 吉川 京燦

WEKO 690017

en 吉川 京燦

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谷本 克之

× 谷本 克之

WEKO 690018

en 谷本 克之

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黒岩 俊隆

× 黒岩 俊隆

WEKO 690019

en 黒岩 俊隆

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石井 徳幸

× 石井 徳幸

WEKO 690020

en 石井 徳幸

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吉田 英治

× 吉田 英治

WEKO 690021

en 吉田 英治

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山谷 泰賀

× 山谷 泰賀

WEKO 690022

en 山谷 泰賀

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村山 秀雄

× 村山 秀雄

WEKO 690023

en 村山 秀雄

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大橋 靖也

× 大橋 靖也

WEKO 690024

en 大橋 靖也

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桃原 幸子

× 桃原 幸子

WEKO 690025

en 桃原 幸子

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溝江 純悦

× 溝江 純悦

WEKO 690026

en 溝江 純悦

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鎌田 正

× 鎌田 正

WEKO 690027

en 鎌田 正

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渡邊 和洋

× 渡邊 和洋

WEKO 690028

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抄録
内容記述タイプ Abstract
内容記述 [Purpose]Detectingthe distribution of positron emitter generated by nuclear fragmentationreaction in carbon ion beam therapy (auto-activation) applied at Heavy IonMedical Accelerator in Chiba (HIMAC) by means of positron emission tomography(PET) is novel method for therapy quality assurance especially assessingirradiated area. In clinical auto-activation PET settings, we have experienceda significant difference of image quality between LSO-based PET system andBGO-based PET system. Therefore, we planned and performed some phantomexperiments to compare PET scanner performance to image infinitesimalradioactivity. [Methods]Four different PET scanners were used; EXACT HR+,Biograph 16 HiRez (CTI-Siemens), SET-3000 GX/T (Shimadzu corp.) and jPET D4which provides four-layer-depth-of-interaction (DOI) measurement. The crystaldetector materials of each PET scanner were as follows: BGO, LSO, GSO and GSOwith DOI, respectively. A phantom was filled with 18F solution, and scannedevery 6hr until its radioactivity was decayed to the level of the infinitesimalradioactivity generated in clinical auto-activation PET settings. After CT scanor transmission scan for attenuation correction, emission scan was acquired for40min in 3D mode. The emission images were reconstructed by either FBP or OSEM.Reconstructed images were evaluated by visually.[Result]Image quality of thephantom became worse according to the decay of 18F. In particular, imagequality degraded severely when scanned with LSO-based PET system compared tothe others. GSO-based PET system improved the image of infinitesimal radioactivitybetter compared to that of BGO-PET system, because sensitivity of GSO-based PETsystem was 2-fold-higher than BGO-based PET system. Additionally, jPET D4 whichwas one of GSO-based PET system performed best in image quality for 18F phantomstudy due to high sensitivity derived from DOI measurement. The randomcoincidence events of LSO-based PET system were 1M counts when itsradioactivity was almost equally to clinical auto-activation settings, whilethe true coincidence was 0.2M counts. The true/random ratio was 24.3%, bycontrast, that of other PET systems was 99.9%. The reason why serious imagedegradation occurred when scanned with LSO-based PET system might be due topresence of 176Lu in LSO crystals[Conclusion]According to analysis of coincidenceevents, LSO-based PET system was not suitable for detecting infinitesimalradioactivity due to intrinsic radioactivity of 176Lu. An evaluation of imagequality suggested that high sensitive PET system, like jPET D4, was necessaryto detect infinitesimal radioactivity. To image the auto-activation using PETscanner, we must take characteristics of crystals and sensitivity of PET systeminto consideration.
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 EANM Annual Congress 2010
発表年月日
日付 2010-10-13
日付タイプ Issued
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