Ter-Pogossian M M
Semin Nucl Med. 1977 Apr;7(2):109-27. doi: 10.1016/s0001-2998(77)80013-5.
Computer tomography (CT) is a radiological imaging method which yields transverse tomographic images reflecting with high accuracy the spatial distribution of x-ray attenuation in the part examined. The contrast resolution achieved by CT permits the visualization of soft tissue structure heretofore invisible with conventional radiographic procedure. The CT image is reconstructed by a computer applied algorithm, from a series of x-ray attenuation measurements obtained at different angles around the subject, by means of radiation detectors; The signal to noise ratio for these measurements is optimized by reducing the contribution of scattered radiation and of system noise. The CT principle of image reconstruction is also applicable in nuclear medicine imaging, with the goal of achieving contrast improvement and quantitative assessment of radionuclide distribution over conventional "projection" techniques. In this application, however, the attenuation of the radiation in the tissue interposed between the radionuclide and the detector must be taken into account to yield quantitatively accurate images. Furthermore, the variation of the field of view of the collimator as a function of distance contributes another unwanted variable to the reconstruction process. A mathematically rigorous tomographic reconstruction which would account for these variables is unavailable for gamma ray-emitting radionuclides, although approximate solutions of that problem have led to the satisfactory images of the head. Images of larger inhomogeneous organs are less quantitative. The detection of coincidence annihilation counting of positron-emitting radionuclides allows the accurate correction for the attenuation of that radiation in tissues and permits depth independent collimation which renders these radionuclide particularly suitable for their imaging by CT. A number of CT devices designed for the imaging of positron emitting radionuclides are yielding nuclear medicine images of quality and potential clinical usefulness unequaled by more conventional projection techniques.
计算机断层扫描(CT)是一种放射成像方法,它能产生横向断层图像,高精度地反映被检查部位X射线衰减的空间分布。CT所实现的对比分辨率使得软组织结构得以可视化,而这些结构在传统放射照相程序中是无法看到的。CT图像是通过计算机应用算法,根据围绕受试者在不同角度通过辐射探测器获得的一系列X射线衰减测量值重建而成的;通过减少散射辐射和系统噪声的影响,优化了这些测量的信噪比。CT图像重建原理也适用于核医学成像,目的是在传统“投影”技术的基础上提高对比度并对放射性核素分布进行定量评估。然而,在这种应用中,必须考虑介于放射性核素和探测器之间的组织中辐射的衰减,以获得定量准确的图像。此外,准直器视场随距离的变化给重建过程带来了另一个不必要的变量。对于发射γ射线的放射性核素,目前还没有一种能考虑这些变量的数学上严格的断层重建方法,尽管对该问题的近似解已能得到令人满意的头部图像。对于更大的不均匀器官的图像,定量程度较低。正电子发射放射性核素的符合湮灭计数检测能够对该辐射在组织中的衰减进行精确校正,并允许进行与深度无关的准直,这使得这些放射性核素特别适合通过CT进行成像。一些专为正电子发射放射性核素成像设计的CT设备所产生的核医学图像,其质量和潜在临床实用性是更传统的投影技术所无法比拟的。