Automatic high‐order shimming using parallel columns mapping (PACMAP)

This work presents a new automatic high‐order shimming method that maps the B0 field using a group of parallel columns. We found that a pair of four columns in two separate slices could determine an optimal correction field comprising the spherical harmonic terms up to the third‐order. The technique of multiple stimulated echoes was incorporated into the method, allowing the use of at least eight shots to accomplish field mapping. The shim currents were first determined in the logic frame by assuming that the slices were in axial planes, and then uniquely converted into the physical frame where the slices could be at any oblique angle, by using a spherical harmonics rotation transformation. This method thus works regardless of slice orientation. It was demonstrated on a 3T scanner equipped with a complete set of second‐order harmonic shim coils. Both phantom and in vivo experiments showed that this newly introduced high‐order shimming method is an effective and efficient way to reduce field inhomogeneity for a region of imaging slices. Magn Reson Med, 2009. © 2009 Wiley‐Liss, Inc.

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

[2]  Hoby P Hetherington,et al.  Fully automated shim mapping method for spectroscopic imaging of the mouse brain at 9.4 T , 2006, Magnetic resonance in medicine.

[3]  T. L. Davis,et al.  Automated shimming at 1.5 t using echo‐planar image frequency maps , 1995, Journal of magnetic resonance imaging : JMRI.

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

[5]  Mark S. Gordon,et al.  Rapid and stable determination of rotation matrices between spherical harmonics by direct recursion , 1999 .

[6]  G. Glover,et al.  Regularized higher‐order in vivo shimming , 2002, Magnetic resonance in medicine.

[7]  Jun Shen,et al.  Measurement and automatic correction of high-order B0 inhomogeneity in the rat brain at 11.7 Tesla. , 2004, Magnetic resonance imaging.

[8]  D. Rothman,et al.  Improvements on an in Vivo automatic shimming method (FASTERMAP) , 1997, Magnetic resonance in medicine.

[9]  Jullie W Pan,et al.  Linear projection method for automatic slice shimming , 1999, Magnetic resonance in medicine.

[10]  D. Hoult,et al.  Magnet field profiling: Analysis and correcting coil design , 1984, Magnetic resonance in medicine.

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

[12]  R Gruetter,et al.  Field mapping without reference scan using asymmetric echo‐planar techniques , 2000, Magnetic resonance in medicine.

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

[14]  Shigehide Kuhara,et al.  In vivo rapid magnetic field measurement and shimming using single scan differential phase mapping , 1996, Magnetic resonance in medicine.

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

[16]  L Martyn Klassen,et al.  Robust automated shimming technique using arbitrary mapping acquisition parameters (RASTAMAP) , 2004, Magnetic resonance in medicine.

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

[18]  R Gruetter,et al.  Automatic, localized in Vivo adjustment of all first‐and second‐order shim coils , 1993, Magnetic resonance in medicine.

[19]  Terence W Nixon,et al.  Dynamic shim updating (DSU) for multislice signal acquisition , 2003, Magnetic resonance in medicine.