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3.0T体部磁共振成像:了解机遇与挑战

Body MR imaging at 3.0 T: understanding the opportunities and challenges.

作者信息

Barth Mara M, Smith Martin P, Pedrosa Ivan, Lenkinski Robert E, Rofsky Neil M

机构信息

Department of Radiology, Beth Israel Deaconess Medical Center, Boston, MA 02215, USA.

出版信息

Radiographics. 2007 Sep-Oct;27(5):1445-62; discussion 1462-4. doi: 10.1148/rg.275065204.

DOI:10.1148/rg.275065204
PMID:17848702
Abstract

The development of high-field-strength magnetic resonance (MR) imaging systems has been driven in part by expected improvements in signal-to-noise ratio, contrast-to-noise ratio, spatial-temporal resolution trade-off, and spectral resolution. However, the transition from 1.5- to 3.0-T MR imaging is not straightforward. Compared with body imaging at lower field strength, body imaging at 3.0 T results in altered relaxation times, augmented and new artifacts, changes in chemical shift effects, and a dramatic increase in power deposition, all of which must be accounted for when developing imaging protocols. Inhomogeneities in the static magnetic field and the radiofrequency field at 3.0 T necessitate alterations in the design of coils and other hardware and new approaches to pulse sequence design. Techniques to reduce total body heating are demanded by the physics governing the specific absorption rate. Furthermore, the siting and maintenance of 3.0-T MR imaging systems are complicated by additional safety hazards unique to high-field-strength magnets. These aspects of 3.0-T body imaging represent current challenges and opportunities for radiology practice.

摘要

高场强磁共振(MR)成像系统的发展部分得益于预期在信噪比、对比噪声比、时空分辨率权衡以及谱分辨率方面的改善。然而,从1.5T到3.0T MR成像的转变并非一帆风顺。与低场强下的身体成像相比,3.0T的身体成像会导致弛豫时间改变、伪影增多和出现新伪影、化学位移效应变化以及功率沉积显著增加,在制定成像方案时所有这些都必须予以考虑。3.0T时静磁场和射频场的不均匀性使得线圈及其他硬件的设计需要改变,并且需要新的脉冲序列设计方法。控制比吸收率的物理原理要求采用降低全身发热的技术。此外,3.0T MR成像系统的选址和维护因高场强磁体特有的额外安全隐患而变得复杂。3.0T身体成像的这些方面代表了放射学实践当前面临的挑战和机遇。

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