Implementing a two-stage, shim field-calibrated superconducting shimming method on a 7 T cryogen-free small animal MRI magnet

被引:0
作者
Liu, Jinhao [1 ]
Wang, Yaohui [3 ,4 ]
Wang, Miutian [2 ]
Wang, Wenchen [7 ]
Yang, Gang [5 ]
Wang, Weimin [2 ,5 ,6 ]
Wang, Qiuliang [3 ,4 ]
Liu, Feng [7 ]
机构
[1] Xi An Jiao Tong Univ, Sch Elect Engn, Xian 710049, Peoples R China
[2] Peking Univ, Sch Elect, Beijing 100871, Peoples R China
[3] Univ Chinese Acad Sci, Sch Elect Elect & Commun Engn, Beijing 100190, Peoples R China
[4] Chinese Acad Sci, Inst Elect Engn, Div Superconducting Magnet Sci & Technol, Beijing 100190, Peoples R China
[5] Peking Univ, Shenzhen Grad Sch, Inst Biomed Engn, Shenzhen 518055, Peoples R China
[6] Inst Biomed Engn, Shenzhen Bay Lab, Shenzhen 518132, Peoples R China
[7] Univ Queensland, Sch Informat Technol & Elect Engn, Brisbane, Qld 4072, Australia
基金
美国国家科学基金会;
关键词
Superconducting shimming; Two-stage method; Ultrahigh field (UHF); Magnetic resonance imaging (MRI); Peak-to-peak homogeneity; HUMAN BRAIN; GRADIENT; DISTORTION; DESIGN;
D O I
10.1016/j.jmr.2024.107787
中图分类号
Q5 [生物化学];
学科分类号
071010 ; 081704 ;
摘要
Ultrahigh field systems (>= 7 T) can increase the signal-to-noise ratio of magnetic resonance imaging (MRI), improving imaging performance compared to systems with lower fields. However, these enhancements heavily rely on a high B 0 magnetic field homogeneity level, which can be achieved through superconducting shimming. This paper presents a novel two-stage superconducting shimming method designed to achieve precise shimming for a 7 T MRI superconducting magnet. In the initial stage, detailed measurements and fittings were conducted to determine the current polarity and the axial or circumferential positions of the shim fields. Subsequently, an optimization strategy was implemented to determine the optimal shim currents with a flexible target field. The second stage involves an iterative process to fine-tune the current of a specific shim coil, identified as having the most significant impact on field homogeneity. The overall fitness of 99.5% underscores the precision in determining the current polarity and position of the shim fields. Significantly, the calibrated shim system substantially improves the peak-to-peak and Root Mean Square Error (RMSE) field homogeneities from 107.42 ppm and 37.00 ppm to 11.12 ppm and 3.26 ppm, respectively, representing improvements of 89.65% and 91.19%. Furthermore, the simulation results of the fine-tuning stage demonstrate additional enhancements in peak-to-peak field homogeneity, to 9.9 ppm by reducing the current of the Z2 shim coil by 51.3 mA. Additionally, the shimmed magnetic field exhibited high time stability, with a maximum variation of only 27 mu T observed within 48 h. Thus, the proposed two-stage superconducting shimming framework effectively addresses the challenge of imperfect B 0 magnetic fields, enhancing peak-to-peak and RMSE field homogeneity. The stepwise optimized approach also mitigates deviations caused by shim-to-shim coupling, demonstrating its efficacy in achieving precise shimming in ultrahigh-field MRI systems.
引用
收藏
页数:11
相关论文
共 51 条
[1]   Field Mapping and Automated Shimming of an HTS Magnet by "Internal" Active Shim Coils Located in the Bore of the Magnet [J].
Ahn, Min Cheol ;
Jang, Jeongwoo ;
Hahn, Seungyong ;
Kim, Young-Gyun ;
Lee, Haigun .
IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 2015, 25 (03)
[2]   3-D Field Mapping and Active Shimming of a Screening-Current-Induced Field in an HTS Coil Using Harmonic Analysis for High-Resolution NMR Magnets [J].
Ahn, Min Cheol ;
Hahn, Seungyong ;
Lee, Haigun .
IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 2013, 23 (03)
[3]   PASSIVE SHIMMING OF THE SUPERCONDUCTING MAGNET FOR MRI [J].
BELOV, A ;
BUSHUEV, V ;
EMELIANOV, M ;
EREGIN, V ;
SEVERGIN, Y ;
SYTCHEVSKI, S ;
VASILIEV, V .
IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 1995, 5 (02) :679-681
[4]  
Blasche M., 2017, Magnet Homogeneity and Shimming
[5]   Principles, Techniques, and Applications of T2*-based MR Imaging and Its Special Applications [J].
Chavhan, Govind B. ;
Babyn, Paul S. ;
Thomas, Bejoy ;
Shroff, Manohar M. ;
Haacke, E. Mark .
RADIOGRAPHICS, 2009, 29 (05) :1433-U272
[6]   Active shimming method for a 21.3 MHz small-animal MRI magnet [J].
Chen, Shanshan ;
Xia, Tian ;
Miao, Zhiying ;
Xu, Luoyuan ;
Wang, Hongzhi ;
Dai, Shuguang .
MEASUREMENT SCIENCE AND TECHNOLOGY, 2017, 28 (05)
[7]   Progress of the 9.4-T Whole-Body MRI Superconducting Coils Manufacturing [J].
Cheng, Junsheng ;
Li, Lankai ;
Wang, Hui ;
Li, Yi ;
Sun, Wanshuo ;
Chen, Shunzhong ;
Zhao, Baozhi ;
Zhu, Xucheng ;
Wang, Lei ;
Dai, Yinming ;
Yan, Luguang ;
Wang, Qiuliang .
IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 2018, 28 (04)
[8]   Active Shim Design of a 7 T Highly Homogeneous Superconducting Magnet for Lanzhou Penning Trap [J].
Du, J. J. ;
Yuan, P. ;
Wu, W. ;
Ma, L. Z. ;
Yang, X. L. .
IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 2012, 22 (03)
[9]   FIELD HOMOGENIZING COILS FOR NUCLEAR SPIN RESONANCE INSTRUMENTATION [J].
GOLAY, MJE .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1958, 29 (04) :313-315
[10]   Operation and performance analyses of 350 and 700 MHz low-/high-temperature superconductor nuclear magnetic resonance magnets: A march toward operating frequencies above 1 GHz [J].
Hahn, Seungyong ;
Bascunan, Juan ;
Lee, Haigun ;
Bobrov, Emanuel S. ;
Kim, Wooseok ;
Ahn, Min Cheol ;
Iwasa, Yukikazu .
JOURNAL OF APPLIED PHYSICS, 2009, 105 (02)