Department of Nuclear Medicine, University at Buffalo, SUNY, Buffalo, NY 14214, USA.
Phys Med Biol. 2012 Nov 7;57(21):6827-48. doi: 10.1088/0031-9155/57/21/6827. Epub 2012 Oct 3.
To achieve optimal PET image reconstruction through better system modeling, we developed a system matrix that is based on the probability density function for each line of response (LOR-PDF). The LOR-PDFs are grouped by LOR-to-detector incident angles to form a highly compact system matrix. The system matrix was implemented in the MOLAR list mode reconstruction algorithm for a small animal PET scanner. The impact of LOR-PDF on reconstructed image quality was assessed qualitatively as well as quantitatively in terms of contrast recovery coefficient (CRC) and coefficient of variance (COV), and its performance was compared with a fixed Gaussian (iso-Gaussian) line spread function. The LOR-PDFs of three coincidence signal emitting sources, (1) ideal positron emitter that emits perfect back-to-back γ rays (γγ) in air; (2) fluorine-18 (¹⁸F) nuclide in water; and (3) oxygen-15 (¹⁵O) nuclide in water, were derived, and assessed with simulated and experimental phantom data. The derived LOR-PDFs showed anisotropic and asymmetric characteristics dependent on LOR-detector angle, coincidence emitting source, and the medium, consistent with common PET physical principles. The comparison of the iso-Gaussian function and LOR-PDF showed that: (1) without positron range and acollinearity effects, the LOR-PDF achieved better or similar trade-offs of contrast recovery and noise for objects of 4 mm radius or larger, and this advantage extended to smaller objects (e.g. 2 mm radius sphere, 0.6 mm radius hot-rods) at higher iteration numbers; and (2) with positron range and acollinearity effects, the iso-Gaussian achieved similar or better resolution recovery depending on the significance of positron range effect. We conclude that the 3D LOR-PDF approach is an effective method to generate an accurate and compact system matrix. However, when used directly in expectation-maximization based list-mode iterative reconstruction algorithms such as MOLAR, its superiority is not clear. For this application, using an iso-Gaussian function in MOLAR is a simple but effective technique for PET reconstruction.
为了通过更好的系统建模实现最优的 PET 图像重建,我们开发了一种基于每个响应线(LOR)概率密度函数的系统矩阵(LOR-PDF)。LOR-PDF 根据 LOR 与探测器的入射角分组,形成一个高度紧凑的系统矩阵。该系统矩阵已在小动物 PET 扫描仪的 MOLAR 列表模式重建算法中实现。通过对比恢复系数(CRC)和方差系数(COV),从定性和定量两方面评估了 LOR-PDF 对重建图像质量的影响,并将其与固定高斯(等高斯)线扩散函数的性能进行了比较。推导了三个符合信号发射源的 LOR-PDF:(1)在空气中发射完美背靠背γ射线(γγ)的理想正电子发射体;(2)水中的氟-18(¹⁸F)核素;(3)水中的氧-15(¹⁵O)核素,并使用模拟和实验体模数据对其进行了评估。推导的 LOR-PDF 表现出各向异性和不对称性特征,这取决于 LOR-探测器角度、符合发射源和介质,与常见的 PET 物理原理一致。等高斯函数与 LOR-PDF 的比较表明:(1)在没有正电子射程和共线效应的情况下,对于半径为 4mm 或更大的物体,LOR-PDF 实现了更好或相似的对比度恢复和噪声权衡,并且这种优势在更高的迭代次数下扩展到更小的物体(例如,半径为 2mm 的球体,半径为 0.6mm 的热棒);(2)在存在正电子射程和共线效应的情况下,取决于正电子射程效应的显著性,等高斯函数实现了相似或更好的分辨率恢复。我们得出结论,3D LOR-PDF 方法是生成准确紧凑系统矩阵的有效方法。然而,当直接在基于期望最大化的列表模式迭代重建算法(如 MOLAR)中使用时,其优势并不明显。对于这种应用,在 MOLAR 中使用等高斯函数是一种简单但有效的 PET 重建技术。