论文标题
多能CT中的独特标准
Uniqueness criteria in multi-energy CT
论文作者
论文摘要
多能计算机断层扫描(ME-CT)是一种医学成像方式,旨在从探测X射线的衰减特性中重建材料的空间密度。对于二维或三维空间中的每一行,ME-CT测量值可以写为非线性映射,从该行沿该行的未知密度的积分绘制到与不同X射线源能量源相对应的相等数量或更大数量的能量加权积分。因此,ME-CT重建可能被分解为一个两步过程:(i)可用的能量测量值重建材料密度的线积分; (ii)从其线积分重建密度。步骤(ii)是标准线性X射线CT问题,其可逆性是众所周知的,因此本文着重于步骤(i)。我们表明,ME-CT承认稳定的全局反演,但规定(i)步骤中转换的差异(i)中满足适当的方向约束,使其成为p-matrix。我们引入了定量P功能的概念,使我们能够在确定的和过度确定的(源能量谱比材料数量数量的情况下)得出ME-CT的全球稳定性结果。基于成像应用中(骨,水,对比剂)和良好的源能能谱模型中的标准材料特性的数值模拟表明,ME-CT通常是(始终在我们的模拟中)(i)非全球注射剂,因为它在本地是非注射式(不完全排名),或者(II在全球范围内具有限制性),或者是局部构成的in extive(II)的建议(II上是不同的)。
Multi-Energy Computed Tomography (ME-CT) is a medical imaging modality aiming to reconstruct the spatial density of materials from the attenuation properties of probing x-rays. For each line in two- or three-dimensional space, ME-CT measurements may be written as a nonlinear mapping from the integrals of the unknown densities of a finite number of materials along said line to an equal or larger number of energy-weighted integrals corresponding to different x-ray source energy spectra. ME-CT reconstructions may thus be decomposed as a two-step process: (i) reconstruct line integrals of the material densities from the available energy measurements; and (ii) reconstruct densities from their line integrals. Step (ii) is the standard linear x-ray CT problem whose invertibility is well-known, so this paper focuses on step (i). We show that ME-CT admits stable, global inversion provided that (a well-chosen linear transform of) the differential of the transform in step (i) satisfies appropriate orientation constraints that makes it a P-matrix. We introduce a notion of quantitative P-function that allows us to derive global stability results for ME-CT in the determined as well as over-determined (with more source energy spectra than the number of materials) cases. Numerical simulations based on standard material properties in imaging applications (of bone, water, contrast agents) and well accepted models of source energy spectra show that ME-CT is often (always in our simulations) either (i) non-globally injective because it is non-injective locally (differential not of full rank), or (ii) globally injective as soon as it is locally injective (differentials satisfy our proposed constraints).