Huson F R, Bryan R N, MacKay W W, Herrick R C, Colvin J, Ford J J, Pissanetzky S, Plishker G A, Rocha R, Schmidt W
Texas Accelerator Center, The Woodlands.
Magn Reson Med. 1993 Jan;29(1):25-31. doi: 10.1002/mrm.1910290107.
Strong, extensive magnetic fringe fields are a significant problem with magnetic resonance imaging magnets. This is particularly acute with 4-T, whole-body research magnets. To date this problem has been addressed by restricting an extensive zone around the unshielded magnet or by placing external unsaturated iron shielding around the magnet. This paper describes a solution to this problem which uses superconducting coils closely integrated with fully saturated iron elements. A 4-T, 30-cm-bore prototype, based on this design principle, was built and tested. The 5 G fringe field is contained within 1 meter of the magnet bore along the z axis. Homogeneity of the raw magnetic field is 10 ppm over 30% of the magnet's diameter after passive shimming. Compared with an unshielded magnet, 20% less superconductor is required to generate the magnetic field. Images and spectra are presented to demonstrate the magnet's viability for magnetic resonance imaging and spectroscopy.
强而广泛的磁边缘场是磁共振成像磁体的一个重大问题。对于4T的全身研究磁体来说,这个问题尤为严重。迄今为止,解决这个问题的方法是在未屏蔽的磁体周围限制一个广泛的区域,或者在磁体周围放置外部不饱和铁屏蔽。本文描述了一种解决该问题的方法,该方法使用与完全饱和铁元件紧密集成的超导线圈。基于这一设计原理,制造并测试了一个4T、30厘米孔径的原型。在z轴上,5G的边缘场被限制在距磁体孔1米的范围内。经过被动匀场后,原始磁场在磁体直径的30%范围内的均匀性为10ppm。与未屏蔽的磁体相比,产生磁场所需的超导体减少了20%。文中给出了图像和光谱,以证明该磁体用于磁共振成像和光谱学的可行性。