RF power absorption during MRI, expressed in terms of specific absorption rate (SAR), is an important safety issue, especially in multi-channel transmit MRI. To reduce uncertainties of local SAR estimates due to subject antatomical variations, patient-specific human body models can be applied in EM simulations of the RF transmit coil. In this work, we trained a U-net neural network on simulated CT scans to quickly create HBMs with four primary tissue classes (bone, lungs, fat, and water-based). Local SAR results using HBMs created with the U-net showed good agreement with those from ground truth models.
We trained a U-net neural network using simulated CT images created from a dataset of detailed, whole-body phantoms of the male and female anatomies generated from NURBS-based Cardiac-Torso (NCAT) phantoms2. Fifty-five whole-body simulated scans (33 male, 22 female) were generated3,4. The simulated images were processed to create a segmentation map with four tissue classes—bone, lungs, fat, and water-based tissue—chosen such that all tissues binned into each class share similar permittivity and electrical conductivity5 values. Fig. 1a shows a sample simulated CT image from one of the phantoms, and Fig. 1b shows the manually-labelled tissue class map for the same image. The network architecture shown in Fig. 2 was trained to predict segmentation maps that could be turned into new HBMs.
With a fully-trained network, we created HBMs from both the network-predicted segmentation maps as well as the manually-labelled tissue map representing the ground truth for the model. Full-wave electromagnetic (EM) simulations were performed with Sim4Life (ZMT, Zurich, Switzerland) to predict specific absorption rate (SAR) distributions on both. Computed SAR maps were used as input to a time-dependent Penne's bioheat equation (PBHE)6 for the HBMs created. A standard whole-body 16-rung high-pass birdcage RF coil was modeled with a maximum grid resolution of 2mm x 2mm x 2mm. The coil was tuned to 127.74 MHz and driven in quadrature mode for subsequent simulations. The ground-truth and network-predicted HBMs were each positioned inside the coil before two independent simulations were performed. Simulations were performed with the HBMs landmarked on their glabellas. Thermal simulations were run using 1000W continuous input power for 60 minutes and a Dirichlet boundary condition. The nominal literature values7 for tissue perfusion, metabolic heat terms, permittivity, and electrical conductivity were used for the tissue types in the HBMs.
Figure 2c shows a predicted tissue class map using the network, while Fig. 2d shows the confusion matrix for the classes that are relevant to creating a HBM. The matrix is highly diagonal, with only 3.27% of voxels misclassified. As each class is defined by the electrical properties of the tissues in that class, the type of misclassification as well as the overall frequency of the misclassification impacts the final SAR simulations, especially for confusion between fat and water-based tissue.
The SAR10g calculated for each axial slice along a test phantom is seen in Fig. 3 for one of the HBMs. The SAR10g in the network-predicted HBM (orange line) follows the same trends as the ground-truth HBM (blue line). Fig. 4 shows the peak SAR10g for each coronal pixel and Fig. 5 shows the result of a thermal simulation for the same phantom. The largest difference in the simulation results corresponds with the region that had the largest confusion between the muscle and water-based tissue classes.
The average SAR10g calculated in the 6 HBMs over the region inside the coil was 10.6+/-0.8uW/kg for the ground-truth HBMs, and 11.4+/-1.4uW/kg for the network-generated HBMs, an increase of 6.8% for the network-generated models. In each axial slice, the network-generated HBM predicted a peak SAR value approximately 9% higher than the corresponding slice in the ground-truth HBM. While the results suggest that the network-based prediction tends to overestimate SAR values, data from more HBMs will be needed to characterize the observation. Initial thermal simulations support these trends.
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