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Novel Point-Like Radioactive Source With Spherical Positron Absorber

机译:具有球形正电子吸收器的新型点状放射源

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Purpose: In the conventional techniques for determining the calibration factors of positron emission tomography (PET) scanners, cylindrical water and resin phantoms with radioisotope $^{18} {rm F}$ or $^{68}{rm Ge}/^{68}{rm Ga}$ are used. In these methods, however, the results depend on attenuation and scatter correction. The purpose of this study is to develop a point-like $^{68}{rm Ge}/^{68}{rm Ga}$ radioactive source that can be used to determine the calibration factors of PET scanners without the uncertainty of attenuation and scatter correction. Methods: A spherical absorber design was employed to realize a symmetric angular distribution of emitted annihilation photons. A Geant4-based Monte Carlo simulation code was used to compare physics characteristics of point-like sources with various absorber materials. On the basis of this simulation, a point-like $^{68}{rm Ge}/^{68}{rm Ga}$ source with a spherical aluminum absorber was manufactured. Its radioactivity was calibrated at an accredited national calibration facility. A calibration factor of a clinical PET scanner was then obtained with a point-like source and compared with that obtained by a standard cross-calibration method. Results: The emission probability of 0.511 MeV annihilation photon pairs per positron decay was typically 0.6–0.8. The fraction of background photon pairs was 6–8% in the energy region of 0.4–0.6 MeV. Considering these two figures, lower density materials such as aluminum and pol(ymethyl methacrylate) (PMMA) were preferable. For the aluminum absorber, a diameter of 8 mm was suitable to prevent positrons from escaping. The calibration factor obtained with the point-like source agreed w-nth that obtained by the standard method within 2–3%. Conclusion: A point-like $^{68}{rm Ge}/^{68}{rm Ga}$ radioactive source was successfully designed, manufactured, and used for determining a calibration factor of a PET scanner. It can be considered a practical tool for calibrating and evaluating the quantitative aspects of PET scanners.
机译:目的:在用于确定正电子发射断层扫描(PET)扫描仪校准因子的常规技术中,具有放射性同位素$ ^ {18} {rm F} $或$ ^ {68} {rm Ge} / ^ {使用68} {rm Ga} $。但是,在这些方法中,结果取决于衰减和散射校正。这项研究的目的是开发类似点的$ ^ {68} {rm Ge} / ^ {68} {rm Ga} $放射源,该放射源可用于确定PET扫描仪的校准因子,而不会造成衰减的不确定性和散射校正。方法:采用球形吸收器设计来实现发射的an灭光子的对称角度分布。使用基于Geant4的蒙特卡洛模拟代码来比较点状源与各种吸收剂材料的物理特性。基于该模拟,制造了具有球形铝吸收体的点状$ ^ {68} {rm Ge} / ^ {68} {rm Ga} $源。它的放射性是在认可的国家校准设施中校准的。然后使用点状光源获得临床PET扫描仪的校准因子,并将其与通过标准交叉校准方法获得的校准因子进行比较。结果:每个正电子衰变的0.511 MeV photo灭光子对的发射概率通常为0.6-0.8。在0.4-0.6 MeV的能量范围内,背景光子对的比例为6-8%。考虑到这两个数字,优选较低密度的材料,例如铝和聚甲基丙烯酸异丁酯(PMMA)。对于铝吸收器,直径为8毫米是合适的,以防止正电子逸出。用点状离子源获得的校准因子在标准方法的2-3%之内与第n位一致。结论:成功设计,制造了点状$ ^ {68} {rm Ge} / ^ {68} {rm Ga} $放射源,并将其用于确定PET扫描仪的校准因子。它可以被认为是用于校准和评估PET扫描仪定量方面的实用工具。

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