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对用于正电子发射断层显像(PET)成像及定量分析的同位素镓-66的物理特性进行的一项研究。

An investigation of the physical characteristics of 66Ga as an isotope for PET imaging and quantification.

作者信息

Graham M C, Pentlow K S, Mawlawi O, Finn R D, Daghighian F, Larson S M

机构信息

Department of Medical Physics, Memorial Sloan-Kettering Cancer Center, New York, New York 10021, USA.

出版信息

Med Phys. 1997 Feb;24(2):317-26. doi: 10.1118/1.597924.

DOI:10.1118/1.597924
PMID:9048374
Abstract

Isotopes commonly used for PET imaging and quantification have a straightforward decay scheme involving "pure" positron (beta +) emission, i.e., 95%-100% beta + abundance, with no additional gamma rays. 66Ga (Emax = 4.2 MeV, T1/2 = 9.5 h) is a member of a category of isotopes with a lower abundance of beta +'s (57%) and a more complicated spectrum involving combinations of gamma rays that are emitted in cascade. These additional gamma rays tend to cause a higher singles rate, resulting in more random coincidence events. The most abundant positron (51.5%) in the spectrum has one of the highest energies considered for PET imaging. For the purpose of monoclonal antibody dosimetry using 66Ga, it is important to verify the quantification in phantoms prior to initiating human studies. A series of quantitative phantom measurements were performed on the PC4600, a head-optimized BGO based scanner with multiple detector rings. Count rate linearity was verified over concentrations ranging from 4.0 kBq/cc to 37 kBq/cc (0.11-1.0 microCi/cc); resolution averaged 16 mm full width half-maximum in the x and y directions in both the direct and cross planes. Axial resolution was 14 mm. The range of the energetic positrons (up to 4.153 MeV, range 7.6 mm in tissue) was verified as a primary source of resolution degradation. Within the limits outlined above, 66Ga is a suitable isotope for use as 66Ga citrate or with monoclonal antibodies in the detection and staging of tumors and other lesions. In addition, the energetic positrons have possible therapeutic applications when used as a monoclonal antibody label.

摘要

常用于正电子发射断层显像(PET)成像和定量分析的同位素具有简单的衰变模式,涉及“纯”正电子(β+)发射,即β+丰度为95%-100%,且无额外的伽马射线。66Ga(Emax = 4.2 MeV,T1/2 = 9.5 h)是一类β+丰度较低(57%)且光谱更复杂的同位素成员,其光谱涉及级联发射的伽马射线组合。这些额外的伽马射线往往会导致更高的单事例率,从而产生更多的随机符合事件。光谱中最丰富的正电子(51.5%)具有PET成像所考虑的最高能量之一。对于使用66Ga进行单克隆抗体剂量测定而言,在启动人体研究之前在体模中验证定量分析非常重要。在PC4600上进行了一系列定量体模测量,PC4600是一台基于锗酸铋(BGO)的头部优化型扫描仪,具有多个探测器环。在浓度范围为4.0 kBq/cc至37 kBq/cc(0.11 - 1.0微居里/立方厘米)内验证了计数率线性;在直接平面和交叉平面的x和y方向上,分辨率平均为半高宽16毫米。轴向分辨率为14毫米。高能正电子的射程(高达4.153 MeV,在组织中的射程为7.6毫米)被确认为分辨率下降的主要来源。在上述限定范围内,66Ga是一种适合用作柠檬酸66Ga或与单克隆抗体一起用于肿瘤和其他病变检测及分期的同位素。此外,当用作单克隆抗体标记时,高能正电子具有潜在的治疗应用。

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