• Acta Physica Sinica
  • Vol. 68, Issue 19, 198301-1 (2019)
Qing-Ming Huang1、2、3、4, Shan-Shan Chen2、3, Jian-Qing Zhang2、3, Yang Yang2, and Gang Zheng1、4、*
Author Affiliations
  • 1School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
  • 2School of Medical Imaging, Shanghai University of Medicine and Health Sciences, Shanghai 201318, China
  • 3Shanghai Key Laboratory of Molecular Imaging, Shanghai University of Medicine and Health Sciences, Shanghai 201318, China
  • 4Laboratory of Medical Imaging Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
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    DOI: 10.7498/aps.68.20190612 Cite this Article
    Qing-Ming Huang, Shan-Shan Chen, Jian-Qing Zhang, Yang Yang, Gang Zheng. Method of designing magnetic resonance active shimming coil based on target field point method and flow function[J]. Acta Physica Sinica, 2019, 68(19): 198301-1 Copy Citation Text show less
    Design algorithm flow of active shimming coil based on target field and flow function.目标场及流函数结合的有源匀场线圈设计算法流程
    Fig. 1. Design algorithm flow of active shimming coil based on target field and flow function.目标场及流函数结合的有源匀场线圈设计算法流程
    Flow function distribution and coil winding of each order coils: (a) Flow function distribution and coil winding of X and Y coil; (b) flow function distribution and coil winding of Z coil; (c) flow function distribution and coil winding of XY coil; (d) flow function distribution and coil winding of XZ and YZ coil; (e) flow function distribution and coil winding of Z2 coil各阶次线圈的流函数和绕线分布 (a) X, Y线圈的流函数和绕线分布; (b) Z线圈的流函数和绕线分布; (c) XY线圈的流函数和绕线分布; (d) XZ, YZ线圈的流函数和绕线分布; (e) Z2线圈的流函数和绕线分布
    Fig. 2. Flow function distribution and coil winding of each order coils: (a) Flow function distribution and coil winding of X and Y coil; (b) flow function distribution and coil winding of Z coil; (c) flow function distribution and coil winding of XY coil; (d) flow function distribution and coil winding of XZ and YZ coil; (e) flow function distribution and coil winding of Z2 coil 各阶次线圈的流函数和绕线分布 (a) X, Y线圈的流函数和绕线分布; (b) Z线圈的流函数和绕线分布; (c) XY线圈的流函数和绕线分布; (d) XZ, YZ线圈的流函数和绕线分布; (e) Z2线圈的流函数和绕线分布
    FID signal detected by magnetic resonance before and after shimming with active shimming coil: (a) Experimental platform of active shimming coil applied to magnetic resonance system; (b) FID signal before shimming; (c) FWHM of the pre-shimming spectrum; (d) FID signal after the second-order shimming coil shimming; (e) FWHM of after the second-order shimming coil shimming采用有源匀场线圈匀场前后磁共振检测的FID信号和频谱的FWHM (a)有源匀场线圈应用于磁共振系统的实验平台; (b)匀场前FID信号; (c)匀场前频谱的FWHM; (d)二阶匀场线圈匀场后的FID信号; (e)二阶匀场线圈匀场后频谱的FWHM
    Fig. 3. FID signal detected by magnetic resonance before and after shimming with active shimming coil: (a) Experimental platform of active shimming coil applied to magnetic resonance system; (b) FID signal before shimming; (c) FWHM of the pre-shimming spectrum; (d) FID signal after the second-order shimming coil shimming; (e) FWHM of after the second-order shimming coil shimming采用有源匀场线圈匀场前后磁共振检测的FID信号和频谱的FWHM (a)有源匀场线圈应用于磁共振系统的实验平台; (b)匀场前FID信号; (c)匀场前频谱的FWHM; (d)二阶匀场线圈匀场后的FID信号; (e)二阶匀场线圈匀场后频谱的FWHM
    阶次次序分量系数球坐标系直角坐标系
    ( $r,\;\,\theta,\;\,\phi $) ( $x,\;\,y,\;\,z$)
    00Z0A0111
    10Z2A02rcos⁡θz
    11X3A12rsin⁡θ cosϕx
    11Y3B12rsin⁡θ sinϕy
    20Z23A03r2 (3cos2θ–1)/2 z2–(x2+y2)/2
    21XZ12A13r2 cos ⁡θ sinθcosϕxz
    21YZ12B13${r^2}\cos \theta {\rm{sin}}\theta {\rm{sin}}\phi $yz
    22X2Y215A23${r^2}{\rm{si}}{{\rm{n}}^2}\theta {\rm{cos}}2\phi $x2y2
    222XY15B23${r^2}{\rm{si}}{{\rm{n}}^2}\theta {\rm{sin}}2\phi $2xy
    30Z34A04${r^3}\cos \theta (5{\cos ^2}\theta - 3)/2$$z[{z^2} - 3\left( {{x^2} + {y^2}} \right)/2]$
    31XZ215A14${r^3}\sin \theta \cos \phi (5{\cos ^2}\theta - 1)/2$$x[4{z^2} - \left( {{x^2} + {y^2}} \right)]$
    31YZ215B14${r^3}\sin \theta \sin \phi (5{\cos ^2}\theta - 1)/2$$y[4{z^2} - \left( {{x^2} + {y^2}} \right)]$
    32Z(X2Y2) 90A24${r^3}{\rm{cos}}\theta {\rm{si}}{{\rm{n}}^2}\theta {\rm{cos}}2\phi $z(x2y2)
    32XYZ90B24${r^3}{\rm{cos}}\theta {\rm{si}}{{\rm{n}}^2}\theta {\rm{sin}}2\phi $2xyz
    33X3105A34${r^3}{\rm{si}}{{\rm{n}}^3}\theta {\rm{cos}}3\phi $${x^3} - 3x{y^2}$
    33Y3105B34${r^3}{\rm{si}}{{\rm{n}}^3}\theta {\rm{sin}}3\phi $$3{x^2}y - {y^3}$
    40Z45A05/8 ${r^4}(35{\cos ^4}\theta - 30{\rm{co}}{{\rm{s}}^2}\theta + 3)$$8{z^4} - 24{z^2}\left( {{x^2} + {y^2}} \right) + 3{\left( {{x^2} + {y^2}} \right)^2}$
    … …
    Table 1. Component representation of in Cartesian and spherical coordinates. 在直角坐标系和球坐标系下的分量表示
    有源匀场线圈FID信号(积分区域)频谱半高宽/Hz磁场均匀性/ppm
    匀场前127068333819.17
    一阶线圈匀场39373259818.23
    二阶线圈匀场4866520481.98
    Table 2. Comparison of technical indicators for evaluating shimming effect of active shimming coil.
    Qing-Ming Huang, Shan-Shan Chen, Jian-Qing Zhang, Yang Yang, Gang Zheng. Method of designing magnetic resonance active shimming coil based on target field point method and flow function[J]. Acta Physica Sinica, 2019, 68(19): 198301-1
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