Characterization of B0-field fluctuations in prostate MRI
Author(s) -
Lebina S. Kakkar,
Muhammad Usman,
Simon Arridge,
Alex Kirkham,
David Atkinson
Publication year - 2020
Publication title -
physics in medicine and biology
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.312
H-Index - 191
eISSN - 1361-6560
pISSN - 0031-9155
DOI - 10.1088/1361-6560/abbc7f
Subject(s) - nuclear magnetic resonance , prostate cancer , parametric statistics , magnetic resonance imaging , prostate , characterization (materials science) , saturation (graph theory) , spectroscopy , nuclear magnetic resonance spectroscopy , in vivo magnetic resonance spectroscopy , diffusion mri , computer science , medical physics , nuclear medicine , medicine , physics , optics , radiology , cancer , mathematics , statistics , combinatorics , quantum mechanics
Multi-parametric MRI is increasingly used for prostate cancer detection. Improving information from current sequences, such as T2-weighted and diffusion-weighted (DW) imaging, and additional sequences, such as magnetic resonance spectroscopy (MRS) and chemical exchange saturation transfer (CEST), may enhance the performance of multi-parametric MRI. The majority of these techniques are sensitive to B 0 -field variations and may result in image distortions including signal pile-up and stretching (echo planar imaging (EPI) based DW-MRI) or unwanted shifts in the frequency spectrum (CEST and MRS). Our aim is to temporally and spatially characterize B 0 -field changes in the prostate. Ten male patients are imaged using dual-echo gradient echo sequences with varying repetitions on a 3 T scanner to evaluate the temporal B 0 -field changes within the prostate. A phantom is also imaged to consider no physiological motion. The spatial B 0 -field variations in the prostate are reported as B 0 -field values (Hz), their spatial gradients (Hz/mm) and the resultant distortions in EPI based DW-MRI images ( b -value = 0 s/mm 2 and two oppositely phase encoded directions). Over a period of minutes, temporal changes in B 0 -field values were ≤19 Hz for minimal bowel motion and ≥30 Hz for large motion. Spatially across the prostate, the B 0 -field values had an interquartile range of ≤18 Hz (minimal motion) and ≤44 Hz (large motion). The B 0 -field gradients were between −2 and 5 Hz/mm (minimal motion) and 2 and 12 Hz/mm (large motion). Overall, B 0 -field variations can affect DW, MRS and CEST imaging of the prostate.
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