Abstract

High-resolution isotropic T2 mapping of the human brain with multi-echo spin-echo (MESE) acquisitions is challenging. When using a 2D sequence, the resolution is limited by the slice thickness. If used as a 3D acquisition, specific absorption rate limits are easily exceeded due to the high power deposition of nonselective refocusing pulses. A method to reconstruct 1-mm3 isotropic T2 maps is proposed based on multiple 2D MESE acquisitions. Data were undersampled (10-fold) to compensate for the prolonged scan time stemming from the super-resolution acquisition. The proposed method integrates a classical super-resolution with an iterative model-based approach to reconstruct quantitative maps from a set of undersampled low-resolution data. The method was tested on numerical and multipurpose phantoms, and in vivo data. T2 values were assessed with a region-of-interest analysis using a single-slice spin-echo and a fully sampled MESE acquisition in a phantom, and a MESE acquisition in healthy volunteers. Numerical simulations showed that the best trade-off between acceleration and number of low-resolution datasets is 10-fold acceleration with 4 acquisitions (acquisition time = 18 min). The proposed approach showed improved resolution over low-resolution images for both phantom and brain. Region-of-interest analysis of the phantom compartments revealed that at shorter T2 , the proposed method was comparable with the fully sampled MESE. For the volunteer data, the T2 values found in the brain structures were consistent across subjects (8.5-13.1 ms standard deviation). The proposed method addresses the inherent limitations associated with high-resolution T2 mapping and enables the reconstruction of 1 mm3 isotropic relaxation maps with a 10 times faster acquisition.

Highlights

  • Spin-spin relaxation characterised by its relaxation time T2 is one of the two principal relaxation mechanisms in Magnetic Resonance Imaging (MRI)

  • Numerical Simulation Numerical noiseless T2 and PD maps were generated from a segmentation of grey matter (GM), white matter (WM) and cerebrospinal fluid (CSF) in a single axial slice (1x1 mm2 resolution) of a numerical phantom [28]

  • Numerical Phantom T2 maps and images obtained from the SR model-based reconstruction in the numerical phantom using different orientations are shown in Figure 3 in comparison to the ground truth

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Summary

Introduction

Spin-spin relaxation characterised by its relaxation time T2 is one of the two principal relaxation mechanisms in Magnetic Resonance Imaging (MRI). Typically referred to as T2 mapping, provides important information about the tissue of interest. T2 is measured by sequentially acquiring several spin-echo (SE) images, each with a different echo time (TE) and subsequently fitting a mono-exponential decay. This is commonly acknowledged as a gold standard despite residual diffusion effects affecting the T2 quantification. The multiple-echo spin-echo (MESE) sequence in the Carr-Purcell-Meiboom-Gill (CPMG) condition [5] uses subsequent refocusing pulses to acquire multiple echoes for each excitation, reducing the total acquisition length. The imperfect refocusing results in the formation of stimulated (secondary) echoes that disrupt the T2 decay of the primary spin echoes [6]. More complex signal models are required to accurately estimate T2 [6]

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