Department of Radiological Technology, Nagoya University Hospital, 65 Tsurumai-cho, Showa-ku, Nagoya, Aichi, 466-8560, Japan.
Department of Innovative Biomedical Visualization (iBMV), Nagoya University Graduate School of Medicine, 65 Tsurumai-cho, Showa-ku, Nagoya, Aichi, 466-8560, Japan.
Jpn J Radiol. 2022 Sep;40(9):970-978. doi: 10.1007/s11604-022-01281-2. Epub 2022 May 7.
The purpose of this study was to investigate whether the changes in apparent diffusion coefficients (ADCs) due to differences in diffusion time reflect tissue properties in actual measurements of phantoms.
Various n-alkane phantoms and sucrose/collagen phantoms with various collagen densities were set up with and without polyvinyl alcohol (PVA) foam with an average pore diameter of 300 μm. Thus, n-alkanes or sucrose/collagen represented substrate viscosity and the presence of PVA foam represented tissue structure with septum. Diffusion-weighted images with various diffusion times (7.71-60 ms) were acquired using pulsed-gradient spin-echo (PGSE) and oscillating-gradient spin-echo (OGSE) sequences. The ADCs of the phantoms with and without PVA foam were calculated.
The ADCs of some of the phantoms without PVA decreased with diffusion times decreased. In the n-alkane phantoms, only CH showed significantly different ADCs depending on the use of PVA foam in the OGSE sequence. On the other hand, sucrose/collagen phantoms showed significant differences according to diffusion time. The ADCs of the phantoms decreased as the molecular size of the n-alkanes or collagen density of the sucrose/collagen phantom increased. Compared to phantoms without PVA foam, the ADC of the phantoms with PVA foam decreased as the diffusion time increased.
Changes in ADCs due to differences in diffusion time reflect tissue properties in actual measurements of phantoms. These changes in ADCs can be used for tissue characterization in vivo.
本研究旨在探讨扩散时间差异引起的表观扩散系数(ADC)变化是否反映实际测量中组织的特性。
本研究建立了不同 n-烷烃和不同胶原密度的蔗糖/胶原水凝胶模型,其中包括有无平均孔径为 300μm 的聚乙烯醇(PVA)泡沫的模型。因此,n-烷烃或蔗糖/胶原代表了基质黏度,而 PVA 泡沫的存在代表了具有间隔物的组织结构。使用脉冲梯度回波(PGSE)和振荡梯度回波(OGSE)序列获取了不同扩散时间(7.71-60ms)的扩散加权图像。计算了有无 PVA 泡沫的模型的 ADC 值。
一些无 PVA 泡沫的模型的 ADC 值随扩散时间的减少而降低。在 n-烷烃模型中,只有 CH 在 OGSE 序列中使用 PVA 泡沫时表现出显著不同的 ADC 值。另一方面,蔗糖/胶原模型根据扩散时间表现出显著差异。随着 n-烷烃的分子大小或蔗糖/胶原水凝胶模型的胶原密度的增加,模型的 ADC 值降低。与无 PVA 泡沫的模型相比,有 PVA 泡沫的模型的 ADC 值随扩散时间的增加而降低。
扩散时间差异引起的 ADC 变化反映了实际测量中组织的特性。这些 ADC 的变化可用于体内组织特征的描述。