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透射测量期间的辐射暴露:基于CT和锗的技术与当前PET扫描仪的比较

Radiation exposure during transmission measurements: comparison between CT- and germanium-based techniques with a current PET scanner.

作者信息

Wu Tung-Hsin, Huang Yung-Hui, Lee Jason J S, Wang Shih-Yuan, Wang Su-Cheng, Su Cheng-Tau, Chen Liang-Kung, Chu Tieh-Chi

机构信息

Department of Nuclear Science, National Tsing-Hua University, Hsinchu 300, Taiwan, ROC.

出版信息

Eur J Nucl Med Mol Imaging. 2004 Jan;31(1):38-43. doi: 10.1007/s00259-003-1327-6. Epub 2003 Oct 8.

DOI:10.1007/s00259-003-1327-6
PMID:14534833
Abstract

In positron emission tomographic (PET) scanning, transmission measurements for attenuation correction are commonly performed by using external germanium-68 rod sources. Recently, combined PET and computed tomographic (CT) scanners have been developed in which the CT data can be used for both anatomical-metabolic image formation and attenuation correction of the PET data. The purpose of this study was to evaluate the difference between germanium- and CT-based transmission scanning in terms of their radiation doses by using the same measurement technique and to compare the doses that patients receive during brain, cardiac and whole-body scans. Measurement of absorbed doses to organs was conducted by using a Rando Alderson phantom with thermoluminescent dosimeters. Effective doses were calculated according to the guidelines in the International Commission on Radiation Protection Publication Number 60. Compared with radionuclide doses used in routine 2-[fluorine-18]-fluoro-2-deoxy-D-glucose PET imaging, doses absorbed during germanium-based transmission scans were almost negligible. On the other hand, absorbed doses from CT-based transmission scans were significantly higher, particularly with a whole-body scanning protocol. Effective doses were 8.81 mSv in the high-speed mode and 18.97 mSv in the high-quality mode for whole-body CT-based transmission scans. These measurements revealed that the doses received by a patient during CT-based transmission scanning are more than those received in a typical PET examination. Therefore, the radiation doses represent a limitation to the generalised use of CT-based transmission measurements with current PET/CT scanner systems.

摘要

在正电子发射断层扫描(PET)中,通常使用外部锗-68棒源进行用于衰减校正的透射测量。最近,已开发出PET与计算机断层扫描(CT)相结合的扫描仪,其中CT数据可用于解剖代谢图像形成以及PET数据的衰减校正。本研究的目的是通过使用相同的测量技术,评估基于锗和基于CT的透射扫描在辐射剂量方面的差异,并比较患者在脑部、心脏和全身扫描期间所接受的剂量。通过使用带有热释光剂量计的兰多·奥尔德森体模来测量器官的吸收剂量。根据国际辐射防护委员会第60号出版物中的指南计算有效剂量。与常规2-[氟-18]-氟-2-脱氧-D-葡萄糖PET成像中使用的放射性核素剂量相比,基于锗的透射扫描期间吸收的剂量几乎可以忽略不计。另一方面,基于CT的透射扫描的吸收剂量明显更高,尤其是在全身扫描方案中。基于全身CT的透射扫描在高速模式下的有效剂量为8.81 mSv,在高质量模式下为18.97 mSv。这些测量结果表明,患者在基于CT的透射扫描期间接受的剂量超过了典型PET检查中的剂量。因此,辐射剂量是当前PET/CT扫描仪系统中基于CT的透射测量广泛应用的一个限制因素。

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