An in vivo automated shimming method taking into account shim current constraints

Many in vivo imaging techniques require magnetic field homogeneity in the volume of interest. Shim coils of the second and third order spherical harmonics have been used successfully to compensate for complicated field variations caused by the human anatomy itself. The available currents of these coils are invariably limited. In this note we demonstrate that these limits significantly affect the optimal shim condition. We propose an automated in vivo shimming method for arbitrary volumes of interest using 3‐dimensional (3D) field maps. This method is a modification of previous works using least‐squares criteria. The main difference is that a constrained optimization is performed in vivo under the current limits of the shim coils, which improved the field homogeneity significantly over simple truncations of the least‐squares solutions. This shimming method was used with head scans of five normal volunteers on a 4.0 tesla scanner. A fast double‐echo sequence was used to obtain field maps, and a new field uniformity measure was derived for this method. The field mapping sequence was tested against a standard single‐echo Dixon sequence used by previous investigators, and the stability of the shimming method was tested by repeated studies on the same subject.

[1]  B Wood,et al.  A simple field map for shimming , 1987, Magnetic resonance in medicine.

[2]  Philip E. Gill,et al.  Numerical methods for constrained optimization , 1974 .

[3]  G. Glover,et al.  Rapid in vivo proton shimming , 1991, Magnetic resonance in medicine.

[4]  L Axel,et al.  Correction of phase wrapping in magnetic resonance imaging. , 1989, Medical physics.

[5]  H E Rockette,et al.  The effect of image processing on chest radiograph interpretations in a PACS environment. , 1990, Investigative radiology.

[6]  Manfred G Prammer,et al.  A new approach to automatic shimming , 1988 .

[7]  Hitoshi Yamagata,et al.  Automated shimming of B0 for spectroscopic imaging , 1989 .

[8]  C. A. Davis,et al.  The effects of bone on proton NMR relaxation times of surrounding liquids. , 1986, Investigative radiology.

[9]  B. Rosen,et al.  Magnetic susceptibility effects of trabecular bone on magnetic resonance imaging of bone marrow. , 1990, Investigative radiology.

[10]  Eddy-current-compensated field-inhomogeneity mapping in NMR imaging , 1988 .

[11]  Andrew A. Maudsley,et al.  Magnetic field measurement by NMR imaging , 1984 .

[12]  R. Hurd,et al.  Optimized Shimming for High-Resolution NMR Using Three-Dimensional Image-Based Field Mapping , 1994 .

[13]  Rolf Gruetter,et al.  Fast, noniterative shimming of spatially localized signals. In vivo analysis of the magnetic field along axes , 1992 .

[14]  A Hemmingsson,et al.  Measurements of Magnetic Field Variations in the Human Brain Using a 3D‐FT Multiple Gradient Echo Technique , 1995, Magnetic resonance in medicine.

[15]  P Webb,et al.  Rapid, fully automatic, arbitrary‐volume in vivo shimming , 1991, Magnetic resonance in medicine.

[16]  Gary H. Glover,et al.  MR susceptibility misregistration correction , 1993, IEEE Trans. Medical Imaging.

[17]  D. I Hoult “Shimming” on spatially localized signals , 1987 .

[18]  W. T. Dixon Simple proton spectroscopic imaging. , 1984, Radiology.