| Literature DB >> 27092026 |
Frank X Li1, John P Voccio2, Michael Sammartino1, Minchul Ahn2, Seungyong Hahn2, Juan Bascuñán3, Yukikazu Iwasa3.
Abstract
This paper presents a passive shimming design approach for a magic-angle-spinning (MAS) NMR magnet. In order to achieve a 1.5-T magic-angle field in NMR samples, we created two independent orthogonal magnetic vector fields by two separate coils: the dipole and solenoid. These two coils create a combined 1.5-T magnetic field vector directed at the magic angle (54.74° from the spinning axis). Additionally, the stringent magnetic field homogeneity requirement of the MAS magnet is the same as that of a solenoidal NMR magnet. The challenge for the magic-angle passive shimming design is to correct both the dipole and solenoid magnetic field spherical harmonics with one set of iron pieces, the so-called ferromagnetic shimming. Furthermore, the magnetization of the iron pieces is produced by both the dipole and solenoid coils. In our design approach, a matrix of 2 mm by 5 mm iron pieces with different thicknesses was attached to a thin-walled tube, 90-mm diameter and 40-mm high. Two sets of spherical harmonic coefficients were calculated for both the dipole and solenoid coil windings. By using the multiple-objective linear programming optimization technique and coordinate transformations, we have designed a passive shimming set that can theoretically reduce 22 lower-order spherical harmonics and improve the homogeneity of our MAS NMR magnet.Entities:
Keywords: Ferromagnetic; NMR; linear programming; magic–angle-spinning NMR magnet; shimming
Year: 2016 PMID: 27092026 PMCID: PMC4833395 DOI: 10.1109/TASC.2015.2512540
Source DB: PubMed Journal: IEEE Trans Appl Supercond