首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >Novel method to measure the intrinsic spatial resolution in PET detectors based on monolithic crystals
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Novel method to measure the intrinsic spatial resolution in PET detectors based on monolithic crystals

机译:基于整体晶体的PET探测器固有空间分辨率测量的新方法

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The main aim of this work is to provide a method to retrieve the intrinsic spatial resolution of a gamma-ray detector block based on monolithic crystals within an assembled scanner. This method consists on a discrimination of the data using a software collimation process. The results are compared with an alternative method of separating two detector blocks far enough to produce a "virtual" source collimation due to the geometric constraints on the allowed coincidence event angles.A theoretical model has been deduced to fit the measured light distribution profiles, allowing estimating the detector intrinsic spatial resolution. The detector intrinsic spatial resolution is expected to follow a Gaussian distribution and the positron-emitter source shape, given the small size of a Na-22 source with 0.25 mm in diameter, can be assumed to follow a Lorentzian profile. However, the collimation of the data modifies the source shape that is no longer a pure Lorentzian distribution. Therefore, the model is based on the convolution of a Gaussian shaped distribution (contribution of the detector) and a modified Lorentzian distribution (contribution of the collimated source profile) that takes into account the collimation effect.Three LYSO crystals geometries have been studied in the present work, namely a 10 mm thick trapezoidal monolithic block, and two rectangular monolithic blocks with thicknesses of 15 mm and 20 mm, respectively. All the blocks have size dimensions of 50 mm x 50 mm. The experimental results yielded an intrinsic detector spatial resolution of 0.64 +/- 0.02 mm, 0.82 +/- 0.02 and 1.07 +/- 0.03 mm, for the 10 mm, 15 mm and 20 mm thick blocks, respectively, when the source was placed at the center of the detector. The detector intrinsic spatial resolution was moreover evaluated across one of the axis of each crystal. These values worsen to an average value of 0.68 +/- 0.04 mm, 0.90 +/- 0.14 and 1.29 +/- 0.19 mm, respectively, when the whole crystal size is considered, as expected. These tests show an accurate method to determine the intrinsic spatial resolution of monolithic-based detector blocks, once assembled in the PET system.
机译:这项工作的主要目的是提供一种基于组装的扫描仪中的整体晶体来检索伽马射线探测器块的固有空间分辨率的方法。该方法包括使用软件准直过程对数据进行判别。将结果与另一种方法相比较,该方法由于允许的重合事件角度受到几何约束而将两个检测器块分离得足够远,从而产生“虚拟”光源准直。已推导出理论模型以拟合测得的光分布图,从而可以估算探测器的固有空间分辨率。假定直径为0.25 mm的Na-22辐射源的尺寸较小,可以认为探测器的固有空间分辨率遵循高斯分布,而正电子发射源的辐射源形状可以遵循洛伦兹分布。但是,数据的准直会修改源形状,而不再是纯粹的洛伦兹分布。因此,该模型基于考虑了准直效应的高斯形状分布(探测器的贡献)和修正的洛伦兹分布(准直的源轮廓的贡献)的卷积。研究了三种LYSO晶体的几何形状目前的工作,即一个10毫米厚的梯形整体块和两个厚度分别为15毫米和20毫米的矩形整体块。所有块的尺寸均为50 mm x 50 mm。实验结果表明,放置10 mm,15 mm和20 mm厚的块时,固有探测器空间分辨率分别为0.64 +/- 0.02 mm,0.82 +/- 0.02和1.07 +/- 0.03 mm。在探测器的中心。此外,在每个晶体的一个轴上评估了探测器的固有空间分辨率。如预期的那样,当考虑到整个晶体尺寸时,这些值分别恶化为0.68 +/- 0.04mm,0.90 +/- 0.14和1.29 +/- 0.19mm的平均值。这些测试表明,一旦组装到PET系统中,就可以确定单块检测器块固有空间分辨率的准确方法。

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