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. 2022 Sep;88(3):1273-1281.
doi: 10.1002/mrm.29273. Epub 2022 May 12.

Simultaneous high-resolution T2 -weighted imaging and quantitative T2 mapping at low magnetic field strengths using a multiple TE and multi-orientation acquisition approach

Affiliations

Simultaneous high-resolution T2 -weighted imaging and quantitative T2 mapping at low magnetic field strengths using a multiple TE and multi-orientation acquisition approach

Sean C L Deoni et al. Magn Reson Med. 2022 Sep.

Abstract

Purpose: Low magnetic field systems provide an important opportunity to expand MRI to new and diverse clinical and research study populations. However, a fundamental limitation of low field strength systems is the reduced SNR compared to 1.5 or 3T, necessitating compromises in spatial resolution and imaging time. Most often, images are acquired with anisotropic voxels with low through-plane resolution, which provide acceptable image quality with reasonable scan times, but can impair visualization of subtle pathology.

Methods: Here, we describe a super-resolution approach to reconstruct high-resolution isotropic T2 -weighted images from a series of low-resolution anisotropic images acquired in orthogonal orientations. Furthermore, acquiring each image with an incremented TE allows calculations of quantitative T2 images without time penalty.

Results: Our approach is demonstrated via phantom and in vivo human brain imaging, with simultaneous 1.5 × 1.5 × 1.5 mm3 T2 -weighted and quantitative T2 maps acquired using a clinically feasible approach that combines three acquisition that require approximately 4-min each to collect. Calculated T2 values agree with reference multiple TE measures with intraclass correlation values of 0.96 and 0.85 in phantom and in vivo measures, respectively, in line with previously reported brain T2 values at 150 mT, 1.5T, and 3T.

Conclusion: Our multi-orientation and multi-TE approach is a time-efficient method for high-resolution T2 -weighted images for anatomical visualization with simultaneous quantitative T2 imaging for increased sensitivity to tissue microstructure and chemical composition.

Keywords: child brain development; low field MRI; magnetic resonance imaging; pediatric neuroimaging.

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Conflict of interest statement

The authors report no significant financial conflicts of interest with respect to the subject matter of this manuscript.

Figures

FIGURE 1
FIGURE 1
Example illustration of SR image reconstruction using images acquired in the axial, sagittal, and coronal orientations (the frequency encoding/readout and lower resolution directions are labeled) and the final reconstructed image
FIGURE 2
FIGURE 2
Analysis workflow from the acquisition of the source anisotropic T2‐weighted data with coronal, axial, and sagittal orientations (left panel); SR reconstruction of an isotropic T2‐weighted image from the acquired data (bottom, left panel); and calculation of qT2 maps from the aligned and resampled multi‐orientation data (top, right panel). For comparison, qT2 maps calculated from multiple TEs acquired in a single orientation and using Hyperfine‐provided five‐TE approach (middle, right panel) are also shown. As well, we show a multi‐orientation + multi‐TI qT2 calculated from data that was preprocessed using adaptive denoising (bottom, right panel)
FIGURE 3
FIGURE 3
Comparison of qT2 values from four brain regions of interest (top) in each healthy volunteer. Brain regions included cerebellar white matter (green), corpus callosum (light blue), anterior internal capsule (red), and posterior thalamic radiations (dark blue). The ICC between the noise filtered multi‐orientation + multi‐TE and reference Hyperfine 5‐TE qT2 values was 0.93. Example monoexponential fits to the corpus callosum and cerebellar white matter data from one of the healthy volunteers is also shown
FIGURE 4
FIGURE 4
(Left) Comparison of qT2 images through the multi‐element phantom and (Right) Mean phantom multi‐orientation + multi‐TE and reference Hyperfine 5‐TE qT2 values. The solid line corresponds to the line of unity, and errors bars in the phantom measurements denote 1 SD. ICC values for the phantom data were 0.97 (with denoising) and 0.96 (without denoising)

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