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由于低水平外部磁场的影响,旋转 MR 直线加速器设计中的几何变形和匀场考虑。

Geometric distortion and shimming considerations in a rotating MR-linac design due to the influence of low-level external magnetic fields.

机构信息

Department of Medical Physics, Cross Cancer Institute, University of Alberta, Edmonton, Alberta, Canada.

出版信息

Med Phys. 2012 May;39(5):2659-68. doi: 10.1118/1.3702591.

Abstract

PURPOSE

This work investigates with simulation the effect of external stray magnetic fields on a recently reported MRI-linac hybrid, which by design will rotate about the patient axis during therapy. During rotation, interactions with magnetic fields from the earth or nearby ferromagnetic structures may cause unacceptable field distortions in the imaging field of view. Optimal approaches for passive shimming implementation, the degree and significance of residual distortion, and an analysis of the active shimming requirements for further correction are examined.

METHODS

Finite element simulations were implemented on two representative types of biplanar magnet designs. Each of these magnet designs, consisting of a 0.2 T four-post and a 0.5 T C-type unit, was simulated with and without an external field on the order of the earth's field (0.5 G) over a range of rotated positions. Through subtraction, the field distribution resulting from the external field alone could be determined. These measured distributions were decomposed into spherical harmonic components, which were then used to investigate the effect of their selective removal to simulate the effects of passive and active shimming. Residual fields after different levels of shim treatment were measured and assessed in terms of their imaging consequence.

RESULTS

For both magnet types, the overall success of a passive shim implementation was highly dependent on the orientation for which it was based. If this orientation was chosen incorrectly, the passive shim would correct for the induced fields at that location, but the overall maximal distortion at other locations was exacerbated by up to a factor of two. The choice of passive shim orientation with the least negative consequence was found to be that where the magnet B(0) axis and transaxial component of the external field were aligned. Residual fields after passive shimming and frequency offset were found to be low in the simulated scenarios, contributing to <1 mm of distortion for most standard imaging sequences (based on a 0.5 G external field). However, extremely rapid single-shot sequences could be distorted by these residual fields to well over 5 mm. These residuals when analyzed were found to correspond primarily to second-order spherical harmonic terms. One term in particular was found to account for the vast majority of these residual fields, defined by the product of the two axes perpendicular to the axis of rotation. The implementation of this term would allow the resulting geometric distortion to fall to the order of 1 mm, even for single-shot sequences.

CONCLUSIONS

After appropriate passive shimming, the imaging distortion due to an external field of 0.5 G was found to be important only in rapid single-shot sequences, which are especially susceptible to field inhomogeneity. Should it be desirable to use these sequences for real-time tracking, made conceivable due to the lower susceptibility concerns at low field, these residual fields should be addressed. The ability to use only one second-order term for this correction will reduce the cost impact of this decision.

摘要

目的

本研究通过模拟,探讨了一种最近报道的 MRI-直线加速器混合系统在治疗过程中绕患者轴旋转时外部杂散磁场的影响。在旋转过程中,与地磁场或附近铁磁结构的磁场相互作用可能会导致成像视场中不可接受的场畸变。研究了被动匀场实现的最佳方法、残余变形的程度和意义,以及主动匀场校正的分析。

方法

对两种典型的双平面磁体设计进行了有限元模拟。这两种磁体设计均由 0.2 T 四立柱和 0.5 T C 型单元组成,在旋转位置范围内模拟了外加磁场在地球磁场(0.5 G)量级上的影响。通过相减,可以确定仅由外加磁场引起的磁场分布。将这些测量的分布分解为球谐分量,然后用于研究选择性去除它们以模拟被动和主动匀场效果的影响。测量了不同匀场处理水平后的残余场,并根据其对成像的影响进行了评估。

结果

对于两种磁体类型,被动匀场实现的整体成功高度依赖于其基础的取向。如果选择的取向不正确,被动匀场将在该位置校正感应场,但在其他位置的整体最大变形会加剧多达两倍。发现选择对负后果影响最小的被动匀场取向是将磁体 B(0)轴和外加磁场的横轴向对齐。在模拟场景中,被动匀场和频率偏移后的残余场被发现很低,对于大多数标准成像序列(基于 0.5 G 外加磁场),仅导致<1mm 的变形。然而,这些残余场可能会使极其快速的单次激发序列变形超过 5mm。对这些残余场进行分析后发现,它们主要对应于二阶球谐项。发现一个特定的项占这些残余场的绝大部分,由与旋转轴垂直的两个轴的乘积定义。实施该项将使由此产生的几何变形降低到 1mm 以内,即使是在单次激发序列中也是如此。

结论

在外加磁场为 0.5 G 的情况下,经过适当的被动匀场后,发现成像失真仅在快速单次激发序列中很重要,而这些序列特别容易受到磁场不均匀性的影响。如果由于低场时的敏感性降低而希望使用这些序列进行实时跟踪,那么应该解决这些残余场。仅使用一个二阶项进行此校正将降低此决策的成本影响。

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