Marble Andrew E, Mastikhin Igor V, Colpitts Bruce G, Balcom Bruce J
MRI Centre, Department of Physics, P.O. Box 4400, University of New Brunswick, Fredericton, NB, Canada E3B 5A3.
J Magn Reson. 2005 May;174(1):78-87. doi: 10.1016/j.jmr.2005.01.009.
Traditionally, unilateral NMR systems such as the NMR-MOUSE have used the fringe field between two bar magnets joined with a yoke in a 'U' geometry. This allows NMR signals to be acquired from a sensitive volume displaced from the magnets, permitting large samples to be investigated. The drawback of this approach is that the static field (B0) generated in this configuration is inhomogeneous, and has a large, nonlinear, gradient. As a consequence, the sensitive volume of the instrument is both small and ill defined. Empirical redesign of the permanent magnet array producing the B0 field has yielded instruments with magnetic field topologies acceptable for varying applications. The drawback of current approaches is the lack of formalism in the control of B0. Rather than tailoring the magnet geometry to NMR investigations, measurements must be tailored to the available magnet geometry. In this work, we present a design procedure whereby the size, shape, field strength, homogeneity, and gradients in the sensitive spot of a unilateral NMR sensor can be controlled. Our design uses high permeability pole pieces, shaped according to the contours of an analytical expression, to control B0, allowing unilateral NMR instruments to be designed to generate a controlled static field topology. We discuss the approach in the context of previously published design techniques, and explain the advantages inherent in our strategy as compared to other optimization methods. We detail the design, simulation, and construction of a unilateral magnet array using our approach. It is shown that the fabricated array exhibits a B0 topology consistent with the design. The utility of the design is demonstrated in a sample nondestructive testing application. Our design methodology is general, and defines a class of unilateral permanent magnet arrays in which the strength and shape of B0 within the sensitive volume can be controlled.
传统上,诸如NMR-MOUSE之类的单边核磁共振系统使用两个通过轭铁连接成“U”形的条形磁体之间的边缘场。这使得能够从远离磁体的灵敏体积中获取核磁共振信号,从而可以研究大样本。这种方法的缺点是,在这种配置中产生的静磁场(B0)是不均匀的,并且具有大的非线性梯度。因此,仪器的灵敏体积既小又难以确定。对产生B0场的永磁体阵列进行经验性重新设计,已产生了适用于各种应用的磁场拓扑结构的仪器。当前方法的缺点是在B0控制方面缺乏形式化。不是根据核磁共振研究来定制磁体几何形状,而是必须根据现有的磁体几何形状来调整测量。在这项工作中,我们提出了一种设计程序,通过该程序可以控制单边核磁共振传感器灵敏点的大小、形状、场强、均匀性和梯度。我们的设计使用根据解析表达式的轮廓成型的高磁导率极靴来控制B0,从而使单边核磁共振仪器能够设计成产生可控的静磁场拓扑结构。我们在先前发表的设计技术背景下讨论了该方法,并解释了与其他优化方法相比我们策略中固有的优势。我们详细介绍了使用我们的方法设计、模拟和构建单边磁体阵列的过程。结果表明,制造的阵列展现出与设计一致的B0拓扑结构。该设计的实用性在样品无损检测应用中得到了证明。我们的设计方法具有通用性,并定义了一类单边永磁体阵列,其中灵敏体积内B0的强度和形状可以得到控制。