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使用L1范数正则化最小二乘算法对超导磁体进行被动匀场。

Passive shimming of a superconducting magnet using the L1-norm regularized least square algorithm.

作者信息

Kong Xia, Zhu Minhua, Xia Ling, Wang Qiuliang, Li Yi, Zhu Xuchen, Liu Feng, Crozier Stuart

机构信息

Department of Biomedical Engineering, Zhejiang University, Hangzhou, China.

Department of Biomedical Engineering, Zhejiang University, Hangzhou, China; State Key Lab of CAD&CG, Zhejiang University, Hangzhou, China.

出版信息

J Magn Reson. 2016 Feb;263:122-125. doi: 10.1016/j.jmr.2015.11.019. Epub 2016 Jan 8.

Abstract

The uniformity of the static magnetic field B0 is of prime importance for an MRI system. The passive shimming technique is usually applied to improve the uniformity of the static field by optimizing the layout of a series of steel shims. The steel pieces are fixed in the drawers in the inner bore of the superconducting magnet, and produce a magnetizing field in the imaging region to compensate for the inhomogeneity of the B0 field. In practice, the total mass of steel used for shimming should be minimized, in addition to the field uniformity requirement. This is because the presence of steel shims may introduce a thermal stability problem. The passive shimming procedure is typically realized using the linear programming (LP) method. The LP approach however, is generally slow and also has difficulty balancing the field quality and the total amount of steel for shimming. In this paper, we have developed a new algorithm that is better able to balance the dual constraints of field uniformity and the total mass of the shims. The least square method is used to minimize the magnetic field inhomogeneity over the imaging surface with the total mass of steel being controlled by an L1-norm based constraint. The proposed algorithm has been tested with practical field data, and the results show that, with similar computational cost and mass of shim material, the new algorithm achieves superior field uniformity (43% better for the test case) compared with the conventional linear programming approach.

摘要

对于磁共振成像(MRI)系统而言,静磁场B0的均匀性至关重要。被动匀场技术通常用于通过优化一系列钢制匀场片的布局来提高静磁场的均匀性。这些钢片固定在超导磁体内孔的抽屉中,并在成像区域产生一个磁化场,以补偿B0场的不均匀性。实际上,除了场均匀性要求外,用于匀场的钢的总质量应降至最低。这是因为钢质匀场片的存在可能会引入热稳定性问题。被动匀场过程通常使用线性规划(LP)方法来实现。然而,LP方法通常速度较慢,并且在平衡场质量和匀场用钢总量方面也存在困难。在本文中,我们开发了一种新算法,该算法能够更好地平衡场均匀性和匀场片总质量这两个双重约束条件。使用最小二乘法来最小化成像表面上的磁场不均匀性,同时通过基于L1范数的约束来控制钢的总质量。所提出的算法已通过实际场数据进行了测试,结果表明,在计算成本和匀场材料质量相似的情况下,与传统线性规划方法相比,新算法实现了更高的场均匀性(测试案例中提高了43%)。

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