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首页> 外文期刊>Cancer biotherapy and radiopharmaceuticals >Monte carlo modeling of gamma cameras for I-131 imaging in targeted radiotherapy.
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Monte carlo modeling of gamma cameras for I-131 imaging in targeted radiotherapy.

机译:靶向放射疗法中用于I-131成像的伽马相机的蒙特卡洛建模。

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Introduction: Dosimetric studies for targeted radiotherapy require the quantification of activity from scintigraphic images. Quantitative imaging is difficult to achieve because of several effects that can lead to errors in activity estimates, some of which are more apparent when I-131 is considered as a source. An evaluation of these phenomena was performed by modeling the gamma camera and its behavior using Monte Carlo simulations. Two gamma cameras were modeled: DST-XLi and Millennium VG Hawk-Eye (GEMS), and two Monte Carlo codes were used: MCNP (LANL) and GATE (openGate collaboration). GATE is a dedicated single photon emission computed tomography/positron emission tomography (SPECT)/(PET) software based on Geant4 (CERN, Geneve). Materials and Methods: Gamma-camera modeling was performed in 2 steps: first without a collimator, then with a high-energy, all-purpose (HEAP) collimator according to the specifications given by the manufacturer (the simulation took the hexagonal shape of collimator holes into account). Simulated and measured energy spectra from point sources in air were compared (with or without a collimator). Spatial resolution was obtained from line sources in air at various distances from the detector heads. The photons detected in the 20% energy window from a point source were analyzed in order to determine the amount of primary photons, scattered photons (in the collimator), and septal photons (i.e., photons that crossed the collimator septa without interacting). Results: Both codes agree well with experimental measurements for the two gamma cameras considered in this study. This allowed us to validate gamma-camera modeling and also served as a benchmark of GATE (new code) versus MCNP (reference code). As shown previously by Dewaraja et al., septal penetration is an important source of image degradation when HEAP collimators are used for I-131 imaging. With the DST-XLi, and for a point source in air, our simulations have shown that 53% of scattered (30%) and septal penetration (23%) photons are detected in the 20% window. Conclusion: The modeling of two gamma cameras (DST-XLi and Millennium VG Hawk-Eye) has been performed with two Monte Carlo codes (MCNP and Gate). Results obtained with the two Monte Carlo codes agree well with experimental results. As already indicated by several authors, septal penetration and scattered photons in the collimator have a major impact on I-131 scintigraphic imaging.
机译:简介:靶向放射疗法的剂量学研究需要对闪烁显像图像的活性进行量化。定量成像很难实现,因为有几种可能导致活动估计错误的影响,当将I-131视为来源时,其中一些更为明显。通过对伽马相机及其行为进行建模,并使用蒙特卡洛模拟对这些现象进行了评估。对两个伽玛相机进行了建模:DST-XLi和Millennium VG Hawk-Eye(GEMS),并使用了两个蒙特卡洛代码:MCNP(LANL)和GATE(openGate合作)。 GATE是基于Geant4(CERN,日内瓦)的专用单光子发射计算机断层扫描/正电子发射断层扫描(SPECT)/(PET)软件。材料和方法:伽马相机建模分两个步骤进行:首先不使用准直仪,然后根据制造商提供的规格使用高能万能(HEAP)准直仪(模拟采用准直仪的六角形形状)漏洞)。比较了来自空气中点源的模拟和测量的能谱(有或没有准直仪)。从距探测器头不同距离的空气中的线源获得空间分辨率。分析了在20%能量窗口中从点源检测到的光子,以确定初级光子,散射光子(在准直仪中)和隔片光子(即穿过准直器隔片而没有相互作用的光子)的数量。结果:这两个代码与本研究中考虑的两个伽玛相机的实验测量结果非常吻合。这使我们可以验证伽马相机建模,并且还可以作为GATE(新代码)与MCNP(参考代码)的基准。如Dewaraja等人先前所示,当HEAP准直仪用于I-131成像时,间隔穿透是图像退化的重要来源。使用DST-XLi并针对空气中的点源,我们的模拟显示,在20%的窗口中检测到53%的散射光(30%)和隔片穿透光(23%)。结论:已经使用两个蒙特卡洛代码(MCNP和Gate)对两个伽玛相机(DST-XLi和Millennium VG Hawk-Eye)进行了建模。用两个蒙特卡罗编码获得的结果与实验结果非常吻合。正如一些作者已经指出的那样,准直仪中的隔片穿透和散射光子对I-131闪烁显像成像有重大影响。

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