Jürgen Herrler1, Patrick Liebig2, Kurt Majewski3, Rene Gumbrecht2, Dieter Ritter2, Christian Richard Meixner4, Andreas Maier5, Arnd Dörfler1, and Armin Michael Nagel4,6
1Department of Neuroradiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Erlangen, Germany, 2Siemens Healthcare GmbH, Erlangen, Germany, 3Department of Corporate Technology, Siemens, München, Germany, 4Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Erlangen, Germany, 5Department of Computer Science, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Erlangen, Germany, 6Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany
Synopsis
Slice-selective, two-spoke
parallel transmit (pTx) pulses for exciting large flip angles can be designed quickly
and show robust performance for MRI at 7 Tesla using an 8Tx/32Rx coil. Firstly,
clusters of B1+/B0 maps are defined and
corresponding pulses are optimized prior to the scan. These serve as
initialization for a fast, gradient-descent based online-optimization. For each
slice, the best cluster-specific initialization is chosen online via neural
networks, which predict their respective spatial distribution of the
longitudinal magnetization. This approach outperforms other strategies to
initialize the pTx RF pulses such as offline-optimized slab-specific and
circularly polarized RF pulses as initializations.
Introduction
Poor homogeneity
of the transmit (B1+) fields in MRI at 7 Tesla may cause
regions of low signal intensity and contrast variations1. Dynamic parallel transmit (pTx) pulses have shown
great potential to overcome these limitations and produce uniform flip angle
(FA) distributions but are rarely used in a clinical setting due to the
complexity and non-convexity of the pulse design problem2. The concept of Universal Pulses (UPs) has been
proposed and proven to be robust and clinically applicable for a large variety
of applications and body parts3-5. It could also be extended to cases with larger
inter-subject variability using machine learning6. Furthermore, nonselective Fast Online-Customized
(FOCUS) pulses have been proposed for small7 and large8 FA excitations. This method consists of optimizing universal
pulses and parameter values offline, which then enable a robust and quicker individual
online-optimization.
In this work, we show that the FOCUS-concept can be
extended to slice-selective excitation of large FAs despite of largely varying
field patterns. We use the well-established spokes-pulses9, which, however, provide
only few degrees of freedom and may produce signal dropouts in some cases that
currently can only be avoided for small FAs with a specifically developed regularization10.
In this work, we generate clusters of field-maps (all channels’ B1+
and B0 maps) and corresponding UPs. Then we train one neural network
(NN) for each cluster’s UP to predict the longitudinal magnetization (Mz) on every slice, when it is used as initialization for further
individual optimization. Using these NNs, we choose the best possible
initialization among the three cluster-specific pulses. The shown simulations were based on field-maps acquired with a saturation-prepared turbo FLASH sequence using an 8Tx/32Rx RF coil (Nova Medical, Wilmington, USA) at 7 Tesla.Methods
In general, all pulses consisted of 2 spokes
and were optimized using an interior-point method optimization using exact
Hessians to simultaneously optimize the RF shapes and spoke locations11 for a target FA of 80°.
Clustering
This process is illustrated in Figure 1. As a first step, all
transversal slices of in total 20 subjects were interpolated into a universal
3D field of view (FOV). It consisted of 8 universal slab positions with a slab
thickness of 28.6 mm and 4 mm in-plane resolution. All subject’s slices in each
slab were used to optimize a slab-specific UP. In the next step, all slab-specific pulses were
applied on each slice in the dataset. Their resulting FA-NRMSEs were then used
to perform a k-means clustering12. Based on the decrease of the within-cluster sum of squares (WCSS)
value for ascending cluster numbers, we chose K=3 clusters. From
these 3 clusters, we took the 10 slices with the minimum Euclidean distance to
the respective centroid to optimize a cluster-specific UP.
Neural Network training
For each cluster, a NN was trained with the normalized B1+
and B0 maps of 132 subjects, interpolated into the universal FOV’s
x- and y-dimensions. These predict the normalized
spatial distribution of Mz(r) = cos(FA(r)) after an individually optimized pulse
using this cluster’s specific UP as initialization. The NNs were based on a u-net,
originally used for tumor segmentation (https://www.kaggle.com/monkira/brain-mri-segmentation-using-unet-keras), with slight architecture-modifications
and using the magnitude squared error (MSE) as loss. 4173
transversal slices were used for training, 1044 for validation and 580 for
final testing.
Overall Pulse Design Process
Figure 2 shows the
general process of the NN-supported FOCUS pulse design. Prior to the scan, 3
cluster-specific pulses were generated. During the scan, B1+
and B0 maps were acquired and served as input for the NNs to predict
the expected NRMSE when using the different cluster-specific pulses as initialization.
Thereby, one of the cluster-specific pulses is chosen as starting point for the
individual, interior-point method optimization11.
PTx pulses were
evaluated using three different initialization-strategies for the individual
online-optimization under the same local specific absorption rate (SAR)
and peak-voltage constraint: Circularly polarized (CP) pulses and both spokes located in the
center (1), coordinate (CO)-based choice of the 8 slab-specific UPs mentioned above (2)
and NN-based choice of 3 cluster-specific UPs (3).Results
Figure 3 shows the loss
function decrease for different numbers of epochs during the training of one NN,
as well as predictions of Mz for two NNs and corresponding UP-initializations in
one slice. These have shown to be accurate enough to prevent cases with
severely low FAs by choosing a better suitable cluster-specific UP.
Figure 4 shows simulated
FA maps of 6 randomly chosen, exemplary slices of 8 test subjects using the
three mentioned initialization strategies. Figure 5 illustrates the normalized
root mean squared error (NRMSE) of the FA of the same test subjects, averaged over all slices.
The NN-based initialization strategy shows the best homogeneity, followed by CO-based
initializations, which in turn outperforms purely CP initializations.Discussion and Conclusions
NN-supported FOCUS pulses with cluster-specific offline-optimizations robustly
achieve homogeneous, slice-selective, large FA excitations in the head. Yet, strong
B0 offsets lead to bad performances regardless of the initialization. To further improve those, the sinc-shaped
RF sub-pulses could be replaced by ones that provide more ΔB0-robust
excitation patterns in preferably short online-optimization time (e.g. DeepControl13). In general,
this approach can be transferred to other applications and body parts with high
inter-subject variability.Acknowledgements
The authors thank Dr. Ioannis-Angelos Giapitzakis for proofreading and useful suggestions, which helped to improve this abstract.References
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