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磁化球体诱导的溶剂质子横向弛豫:在铁蛋白、红细胞和磁铁矿中的应用

Transverse relaxation of solvent protons induced by magnetized spheres: application to ferritin, erythrocytes, and magnetite.

作者信息

Gillis P, Koenig S H

机构信息

Université de Mons-Hainaut, Belgium.

出版信息

Magn Reson Med. 1987 Oct;5(4):323-45. doi: 10.1002/mrm.1910050404.

Abstract

Since 1/T2 of protons of tissue water is generally much greater than 1/T1 at typical imaging fields, small single-ion contrast agents--such as Gd(DTPA), which make comparable incremental contributions and therefore smaller fractional contributions to 1/T2 compared to 1/T1--are not as desirable for contrast-enhancement as agents that could enhance 1/T2 preferentially. In principle, such specialized agents will only be effective at higher fields because the field dependence (dispersion) of 1/T1 is such that it approaches zero at high fields whereas 1/T2 approaches a constant value. The residual 1/T2 is called the "secular" contribution and arises from fluctuations in time--as sensed by the protons of diffusing solvent or tissue water molecules--of the component of the magnetic field parallel to the static applied field. For solutions or suspensions of sufficiently large paramagnetic or ferromagnetic particles (greater than or equal to 250 A diameter), the paramagnetic contributions to the relaxation rates satisfy 1/T2 much greater than 1/T1 at typical imaging fields. We examine the theory of secular relaxation in some detail, particularly as it applies to systems relevant to magnetic resonance imaging, and then analyze the data for solutions, suspensions, or tissue containing ferritin, erythrocytes, agar-bound magnetite particles, and liver with low-density composite polymer-coated magnetite. In most cases we can explain the relaxation data, often quantitatively, in terms of the theory of relaxation of protons (water molecules) diffusing in the outer sphere environments of magnetized particles. The dipolar field produced by these particles has a strong spatial dependence, and its apparent fluctuations in time as seen by the diffusing protons produce spin transitions that contribute to both 1/T1 and /T2 comparably at low fields; for the larger particles, because of dispersion, the secular term dominates at fields of interest. On the basis of the agreement of theory with data for solutions of small paramagnetic complexes, large magnetite particles, and liver containing low-density polymer-coated magnetite agglomerates, it is argued that the theory is sufficiently reliable so that, e.g., for ferritin--for which 1/T2 is unexpectedly large--the source of its large relaxivity must reside in nonideal chemistry of the ferritin core. For blood, it appears that diffusion through intracellular gradients determines 1/T2.

摘要

由于在典型成像场中,组织水的质子的1/T2通常远大于1/T1,所以小的单离子造影剂——比如钆(二乙三胺五乙酸),其对1/T2的增量贡献与对1/T1的增量贡献相当,因此对1/T2的分数贡献较小——不如那些能优先增强1/T2的造影剂那样适合用于增强对比度。原则上,这种特殊的造影剂仅在更高场强下才有效,因为1/T1的场强依赖性(色散)使得它在高场强时趋近于零,而1/T2趋近于一个恒定值。剩余的1/T2被称为“长期”贡献,它源于与静态外加磁场平行的磁场分量随时间的波动——这种波动由扩散溶剂或组织水分子的质子感知。对于足够大的顺磁性或铁磁性颗粒(直径大于或等于250埃)的溶液或悬浮液,在典型成像场中,顺磁性对弛豫率的贡献满足1/T2远大于1/T1。我们详细研究了长期弛豫理论;尤其考虑了该理论在与磁共振成像相关的系统中的应用,然后分析了含有铁蛋白、红细胞、琼脂结合的磁铁矿颗粒以及低密度复合聚合物包被的磁铁矿的肝脏的溶液、悬浮液或组织的数据。在大多数情况下,我们能够依据质子(水分子)在磁化颗粒外球环境中扩散的弛豫理论,常常是定量地解释弛豫数据。这些颗粒产生的偶极场具有很强的空间依赖性,扩散质子所观察到的其明显的时间波动会产生自旋跃迁,在低场强下对1/T1和1/T2的贡献相当;对于较大的颗粒,由于色散,长期项在感兴趣的场强下占主导。基于理论与小顺磁性络合物溶液、大磁铁矿颗粒以及含有低密度聚合物包被的磁铁矿团聚物的肝脏的数据之间的一致性,有人认为该理论足够可靠,例如对于铁蛋白——其1/T2出人意料地大——其大弛豫率的来源必定在于铁蛋白核心的非理想化学性质。对于血液而言,似乎通过细胞内梯度的扩散决定了1/T2 。

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