We present a new method of artificial neural network (ANN) to suppress metal artifacts in MR Imaging with Slice Encoding for Metal Artifact Correction (SEMAC). Seven titanium‑embedded phantoms were imaged using different SEMAC factors. The acquired data with low and high SEMAC factors were separated into input and label images, respectively, for training. The trained model was tested on separate phantoms. Metal artifacts in low SEMAC factors could be further suppressed visually and quantitatively using the implemented ANN, with the performance being comparable to that of label images. The proposed method reduces scan time necessary for high‑quality SEMAC imaging.
Multilayer Perceptron (MLP) is one of the most commonly used artificial neural network architectures, through which a fully connected hidden layer maps input values into output values. While Convolutional Neural Network (CNN) has become a dominating trend for machine learning, MLP has still proven to be useful for suppressing artifacts in MRI data 3.
In SEMAC technique, extra z-phase encoding steps are implemented for each slice acquisition, from which signals from other z positions (partitions) are acquired and resolved back to their physical locations as a post processing. The number of extra‑encoding steps are called SEMAC factor, and ideally, increasing the factor enhances metal artifact suppression. In this work, low and high SEMAC factor images were categorized into input and ground truth, respectively, and were trained with MLP, through which output images were produced and compared with label images.
Input data were partitions of SEMAC factors 6 and 4, and ground truth data were those of SEMAC factor 12. Partitions of SEMAC factors 4 and 6 were retrospectively acquired from partitions of SEMAC factor 12. We compared partitions of SEMAC factor 6 from the retrospective sampling and those from real acquisition and found no significant difference between the two.
All data acquisitions were performed on a SIEMENS Skyra 3.0 T scanner (Siemens Medical Solutions, Erlangen, Germany). Total of 7 phantoms with different titanium metals embedded in 4% agarose were scanned along multiple directions to collect total 12 image sets. For both SEMAC factors of 6 and 12, proton-density weighted images (PD) were acquired, and the imaging parameters were: TR/TE = 3500.0/34.0 ms, FOV = 180 x 180 mm2, number of slices = 16/18/20 (depending on titanium), slice thickness = 3.0mm, matrix size = 256 x 256, flip angle = 140, and acquisition bandwidth = 610Hz/Px. Two out of total datasets were used for testing and the remaining ten datasets were used for training. This procedure was repeated by changing the two test datasets so that one dataset from every phantom was tested. Normalized root mean square error from the ground truth (NRMSE) was quantified for the analysis of the tested images. Wilcoxon signed rank test was performed to compare NRMSE and p value less than 0.05 was considered statistically significant.
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