High-permittivity pads have proved effective for addressing B1+ inhomogeneities for neuroimaging at 7T and body imaging at 3T. In contrast with the ease of constructing these pads, obtaining an appropriate design involves sophisticated and time-consuming electromagnetic field simulations, meaning that in many applications this technique is not fully exploited. We have therefore developed an easy-to-use software tool which can be run on a standard desktop PC to design dielectric pads for 3T body and 7T neuroimaging applications.
Models
The 7T neuroimaging configuration uses a 15 cm radius high-pass birdcage head coil tuned to 298 MHz. The body model “Duke” from the IT’IS foundation is incorporated on an isotropic grid with a spatial resolution of 5 mm.7 The pad-design domain is defined as a 1 cm thick layer surrounding the head. For the 3T body imaging setup a 128 MHz tuned high-pass birdcage body coil is used, loaded with the same body model “Duke” and discretized on a 7.5 mm isotropic grid. The pad-design domain is defined as a 1.5 cm thick layer around the torso. The body model can be shifted within the birdcage to center different imaging landmarks.
The dielectric pads can be modeled efficiently using diakoptic methods as outlined in previous work.6 To this end, the dynamic pad-design domain is separated from the static full computational domain consisting of the heterogeneous body model and the resonant coils. Subsequently, an offline field response library is computed capturing the static components, such that the online phase only involves the relatively small pad-design domain. The pad model is finally parameterized in terms of the pad’s dimensions, location, and constitution. The methods are illustrated in Figure 1.
The optimization procedure allows one either to find the optimal position of an existing pad, or to find the optimal pad’s geometry, position, and composition. For both procedures the B1+ field can be optimized for either the transmit efficiency, homogeneity, or a combination of both.
Design tool
The stand-alone tool was created in MATLAB (R2015a, The MathWorks, Inc., Natick, Massachusetts, USA) and can run on a standard desktop PC or use a GPU if available to accelerate computations. The tool can be downloaded as an executable file at https://paddesigntool.sourceforge.io.
The graphical user interface for the 7T configuration is shown in Figure 2. The interface allows one to define a three-dimensional ROI by drawing two-dimensional ROIs in the three isometric views at the top. A target B1+ amplitude can be set, or alternatively, an optimization sweep over a range of B1+ amplitudes can be carried out to enable a trade-off analysis between transmit efficiency and B1+ homogeneity. All optimizations can be performed for either one or two pads.
Conclusion
We have designed an easy-to-use software tool to design dielectric pads for 7T neuroimaging and 3T body imaging applications. The application can be downloaded and pads can be designed in a couple of minutes. We anticipate this will help to bridge the gap between the advanced numerical design methods and the practical application by the MR community.1. Yang QX, Mao W, Wang J, et al. Manipulation of image intensity distribution at 7.0 T: Passive RF shimming and focusing with dielectric materials. J Magn Reson Imaging. 2006;24(1):197–202.
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3. de Heer P, Brink WM, Kooij BJ, Webb AG. Increasing signal homogeneity and image quality in abdominal imaging at 3 T with very high permittivity materials. Magn Reson Med. 2012;68(4):1317–1324.
4. Brink WM, Webb AG. High permittivity pads reduce specific absorption rate, improve B 1 homogeneity, and increase contrast-to-noise ratio for functional cardiac MRI at 3 T. Magn Reson Med. 2014;71(4):1632–1640.
5. O’Reilly TPA, Webb AG, Brink WM. Practical improvements in the design of high permittivity pads for dielectric shimming in neuroimaging at 7 T. J Magn Reson. 2016;270:108–114.
6. van Gemert JHF, Brink WM, Webb AG, Remis RF. High-Permittivity Pad Design for Dielectric Shimming in Magnetic Resonance Imaging Using Projection-Based Model Reduction and a Nonlinear Optimization Scheme. IEEE Trans Med Imaging. 2018;37(4):1035–1044.
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