1H-MRS can quantify brain metabolites noninvasively. However, in a typical clinical setting, human brain spectra are indispensably degraded due to low SNR, line-broadening, and unknown spectral baseline, and consequently, quantification of brain metabolites is challenging even with the current state-of-the-art software. Given the recent accomplishment of deep-learning in a variety of different tasks, we developed a convolutional-neural-network (CNN) that maps the degraded brain spectra into noise-free, line-narrowed, baseline-removed, metabolite-only spectra. The robust performance of the proposed method as validated on both simulated and in vivo human brain spectra strongly supports the potential of deep learning in 1H-MRS of human brain.
In a typical clinical setting, brain spectra are degraded due to low SNR, line-broadening, and spectral baseline. To quantify individual metabolites from the degraded brain spectra, a nonlinear least-squares fitting is the most widely used approach.1,2 However, even with the current state-of-the-art software, it is challenging.3 Therefore, development of a robust method for brain metabolite quantification is a remaining issue in 1H-MRS.
Given the recent accomplishment of deep learning in a variety of different tasks, 4,5 we developed a convolutional-neural-network (CNN) that maps degraded in vivo brain spectra into noise-free, line-narrowed, baseline-removed, metabolite-only spectra. The subsequent metabolite quantification from the metabolite-only spectra is achieved by solving a simple inverse problem. The performance of the proposed method was tested on both simulated and in vivo human brain spectra.
In vivo data: The study was approved by IRB (5 healthy volunteers). In vivo spectra were collected from the left frontal lobe using PRESS at 3.0T (Siemens; TR/TE=2000/30ms, SW=2kHz, 2048 points, voxel size=8cm3, and 64 averages).
Brain spectra simulation: Based on the previous studies, 6-9 the upper/lower bounds of the metabolite concentrations in normal human brain were defined for 17 metabolites. First, metabolite-only spectra were simulated by combining all individual metabolite phantom spectra according to randomly varying relative metabolite concentration ratios within the concentration bounds. These metabolite-only spectra were used as the ground-truth target spectra (Fig.1). Second, spectral baseline was simulated by using 17 Gaussian functions with randomly varying relative amplitudes within ±10% from the reported ranges.10,11 Third, the metabolite-only spectra and the baseline spectra were combined by randomly varying their relative ratio within ±10% from a predetermined ratio.12 Forth, line-broadening, noise, and frequency/phase shift were applied to the combined spectra. Finally, 50000 spectra were simulated and assigned to a training (N=40000), a validation (N=5000) and a test (N=5000) sets.
CNN: A CNN was designed and Bayesian-optimized 14 in Matlab (Mathworks Inc) (Fig.1).
Metabolite quantification: The quantification of individual metabolites from the CNN-predicted metabolite-only spectra was achieved by solving an inverse problem. That is, C = S pinv(b) (C: matrix containing the relative concentrations of the 17 metabolites, S: matrix containing the CNN-predicted spectra, pinv: pseudoinverse of a matrix, and b: matrix containing the basis spectra of the 17 metabolites).
Evaluation of the proposed method: Using the simulated spectra in the test set, the proposed method was evaluated by calculating the mean-absolute-percent-error (MAPE) between the ground-truth and the metabolite concentrations estimated by the proposed method. Using in vivo spectra, the quantification results from the proposed method were compared with those from the LCModel analysis.
This research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (2016R1D1A1B03931233), by the Bio & Medical Technology Development Program of the NRF funded by the Korean government, MSIP (NRF-2014M3A9B6069340), by grant no 03-2016-0220 from the SNUH Research Fund, and by the Doosan Yonkang Foundation (30-2017-0120) in Korea.
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