One of the main concerns in fetal MRI is the amount of power that is deposited both in the fetus and the mother. In this work, we show that a well-designed high-permittivity pad can tailor the energy of the RF field such that the transmit efficiency increases and the field becomes more homogeneous. The increase in transmit efficiency subsequently enables a substantial reduction in the SAR in both the mother and the fetus for models of the third, seventh, and ninth months of gestation.
Methods
For the simulations a wide-bore high-pass birdcage coil with a radius of 37.5 cm and tuned to 128 MHz (3T) was used. Pregnant models in the third, seventh, and ninth months of gestation (IT’IS foundation8), are positioned in the bore with either the center or the brain of the fetus placed at magnet isocenter, as shown in Figure 1. The electromagnetic field simulations and SAR evaluations are computed on a uniform and isotropic grid with a resolution of 7.5 mm and 3.75 mm, respectively. Transmit efficiency results were normalized to 1 W input power. Following the approach from other authors (e.g. Murbach et al.3), the SAR results were normalized to 2 W/kg wbSAR.
In previous work,9,10 we developed an efficient approach to design dielectric pads using reduced order modeling and optimization techniques. Following this approach, we define a 1.5 cm thick pad-design domain layer around the belly extending from the groin to just below the breast, as indicated in Figure 1. The optimization techniques allow us to rapidly (~ minutes) determine the optimal pad’s geometry, location, and composition that either provide the highest B1+ homogeneity, expressed in terms of a coefficient of variation (Cv), or the best transmit efficiency in a region of interest (ROI). During the optimization, the width and height of the pad are restricted to 30 cm, the relative permittivity to a maximum of 300, and the conductivity is set to 0.2 S/m.
Two ROIs are evaluated: one encompassing the entire fetus and the other only the brain of the fetus (with the exception of the three months model in which only the entire fetus was possible). The model is placed such that the ROI lies at the magnet isocenter. One set of pads are designed that provide the best Cv and another set that provide the best transmit efficiency.
The SAR is evaluated in terms of avgSAR (the average SAR in a specific body part) and the psSAR10g in the mother, fetus, and the amniotic fluid. The SAR results are normalized with respect to the average B1+ field improvement in the ROI.
The properties of the optimum dielectric pads are displayed in Table 1, where it is shown that a transmit efficiency gain of ~25% can be achieved at 9 months, ~54% at 7 months, and ~45% at 3 months. The Cv decreases in all cases, except for the 9 months case in which the values are very similar.
The B1+ fields and SAR results for the optimum transmit efficiency case are shown in Figure 2, which shows that the spatial distribution of the SAR is very similar to that without dielectric pads. The results show an overall decrease in the SAR values. Specifically, the avgSAR in the mother decreases by more than 31%, 55%, and 53% for the nine, seven, and third months of gestation, respectively. For the optimum Cv case the numbers are slightly lower, i.e. 17, 51% and 53%. Full details are listed in Table 2.
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