Ziener C H, Bauer W R, Jakob P M
Bayerische Julius-Maximilians-Universität Würzburg, Institut für Experimentelle Physik 5, Am Hubland, 97074 Würzburg, Germany.
Magn Reson Med. 2005 Sep;54(3):702-6. doi: 10.1002/mrm.20634.
We describe the NMR relaxation properties of magnetically labeled cells. The cells are labeled with magnetic nanoparticles (SPIO, USPIO), which generate susceptibility contrast. The geometry of the labeled cells and the surrounding tissue is considered. We assume that the magnetic nanoparticles accumulate to form a magnetic core of radius RC inside the cell. The correlation time tau, which describes the motion of spins around this core, is analyzed. Using the strong collision approach, explicit expressions are derived for the transverse relaxation rate R2* for tissue containing labeled cells as a function of the core radius, the diffusion coefficient, and the concentration of the nanoparticles. The predictions of this model agree well with numerical simulations and experimental data.
我们描述了磁性标记细胞的核磁共振弛豫特性。细胞用磁性纳米颗粒(超顺磁性氧化铁纳米颗粒、超小超顺磁性氧化铁纳米颗粒)进行标记,这些颗粒会产生磁化率对比度。我们考虑了标记细胞和周围组织的几何形状。我们假设磁性纳米颗粒在细胞内聚集形成半径为(R_C)的磁核。分析了描述围绕该磁核自旋运动的相关时间(\tau)。使用强碰撞方法,推导出了含有标记细胞的组织横向弛豫率(R2^*)作为磁核半径、扩散系数和纳米颗粒浓度函数的显式表达式。该模型的预测与数值模拟和实验数据吻合良好。