3388

Optimisation of parallel transmission radiofrequency pulses using neural networks
Christopher Mirfin1, Paul Glover1, and Richard Bowtell1

1Sir Peter Mansfield Imaging Centre, School of Physics and Astronomy, University of Nottingham, Nottingham, United Kingdom

Synopsis

Developing fast accurate large-tip-angle radiofrequency pulses and gradient trajectories suitable for ‘online’ use is a challenging problem. In this work we propose a novel method for the sub-second design of RF pulses and gradient trajectories through use of a suitably trained artificial neural network which attempts to learn the required pulse and gradient spoke parameters from B1+ field spatial variations. A method for synthesising a large training database is also described. Our initial results highlight some of the challenges of this approach but suggest areas for future development.

Introduction

At high-field the electromagnetic field distribution becomes inhomogeneous and is highly variable with patient size. Improved uniformity can be achieved for slice-selective excitation through use of spokes1,2; a series of subpulses played-out at different points in k-space. Design of parallel transmit Spokes pulses is complicated further at large-tip-angle due to the inherent nonlinear response of the Bloch equation and additional power and SAR constraints. Existing approaches trade-off target magnetisation accuracy with increased computational time3-8. Developing fast accurate optimisation methods is a major effort to allow ‘online’ pulse and gradient design.

Previous work9 trained a network to design single-channel NMR spectroscopic radiofrequency pulses. In this work we propose a novel method for the sub-second design of RF pulses and gradient trajectories through use of a suitably trained artificial neural network which attempts to learn the required pulse and gradient spoke parameters from B1+ field spatial variations.

Method

To learn the spatial variations of the B1+ channel fields a training set of 60,000 x 8 B1+ maps and optimal solutions was created (see Figure 1). From an initial full electromagnetic field simulation (provided by Nova Medical Inc., Wilmington, USA) of a male human head (downsampled to 25 x 25 voxels) within an 8-channel transmit/32-channel receive coil, individual transmit channel fields were fitted using a near-field dipole approximation over spatial coordinates. Subtraction of these fields resulted in a residual field which was decomposed into its Fourier components. The top 80% of Fourier coefficients were then randomly perturbed 60,000 times according to a normal distribution (0.1 variance) for each of the transmit channels.

Joint optimisation of 5-spoke RF pulses (amplitude and phase) plus gradient trajectory for slice inversion was performed for each of the entries within the B1+ map database, using an optimal control approach with power regularisation (for implementation see3), yielding a set of 90 design parameters (5 x 8 channel amplitude, 5 x 8 channel phases, 5 x 2 k-space locations) for each B1+ map set.

A neural network consisting of an input layer (2056 nodes), hidden layer (1000 nodes) with sigmoidal activation functions, and output layer (90 nodes) was employed. The network weights were iteratively updated using a commercial backpropagation algorithm with conjugate gradient descent (MATLAB, Natwick, USA) to minimise the squared error between the neural network outputs and training design parameters (see Figure 2). The training data was feature scaled and randomly divided towards 70% training, 30% validation.

Results

Creation of the training data (B1+ maps and optimal solutions) took 14 hours to compute using a high-performance computing facility (3 x 16 processors, 2.66 GHz). The optimised k-space 5-spoke locations (see Figure 3) are shown to be distributed in clusters. During the training phase, the number of hidden nodes was adjusted to achieve a balance between training error, cross-validation error and overall training time (18 hours), resulting in a hidden layer of size 1000.

On an unseen set of 10 B1+ maps, the network achieved a root-mean-square error (RMSE) of 0.38±0.04, with an average design time of 0.1 seconds (desktop PC, 3.70 GHz processor). In comparison, applying the full optimal control method achieved a substantially lower 0.06±0.04 RMSE with an average optimisation time of 370 seconds. Drawing a set of parameters directly from the training data yielded a 0.45±0.20 RMSE.

Discussion

We have proposed a new method for the sub-second design of large-tip-angle parallel transmit pulses based on learning the spatial variations within patient field maps. Our initial results show inferior inversion performance as compared to joint-optimisation of Spokes pulses using a full optimal control. We only observe a slight improvement over drawing parameters directly from the training set, suggesting our network design is heavily biased and not able to fully regress the 90 design parameters from the given field maps.

A likely factor in this can be found in Figure 3, demonstrating that the 5-spoke k-space locations for each of the training set entries are located in clusters. This reflects the small perturbation model that was used to create the training data and the down-sampling that was required to reduce the computation time required to create a large database. A potential for future work will be to apply our approach to inversion pulse design for the abdomen – where the degree of B1+ field variation between patients is greater. In addition, increasing the number of nodes and hidden layers in the model will reduce biasing but would require a larger training set to prevent over-fitting.

Acknowledgements

This work was supported by funding from the Engineering and Physical Sciences Research Council (EPSRC) and Medical Research Council (MRC) [grant number EP/L016052/1]. We are grateful for access to the University of Nottingham High Performance Computing Facility.

References

[1] Saekho S. et al. (2005): MRM. 53: 479-484

[2] Saekho S. et al. (2006): MRM. 55: 719-724

[3] Cao Z. et al. (2016): MRM. 75: 1198-1208

[4] Xu D. et al. (2008): MRM. 59: 547-560

[5] Grissom W. et al. (2008): MRM. 59: 779-787

[6] Grissom W. et al. (2009): IEEE Trans Med Imaging. 28: 1548-1559

[7] Setsompop K. et al. (2008): MRM. 195: 76-84

[8] Gras V. et al. (2016): JMR. 261: 181-189

[9] Gezelter J. et al. (1990): JMR. 90: 397-404

Figures

Figure 1. Creation of B1+ example. (a) Input B1+ for kth transmit channel. (b) Produce dipole near-field fit. (c) Produce residual field after subtraction of near-field fit. (d) Fourier transform, perturb components, inverse Fourier transform. (e) Recombine with near-field fit to produce final perturbed field.

Figure 2. Schematic diagram showing training (dashed boxes) and propagation (solid boxes) of neural network. Full network consisted of 2056 input nodes, 1000 hidden nodes, and 90 output nodes. During training the connecting weights between nodes are iteratively adjusted to fit to the training data.

Figure 3. Optimal control optimised k-space locations for training data (60,000 examples) for an 8-channel 5-spoke inversion pulse. The locations form clusters as only small perturbations were allowed in the creation of the B1+ database.

Figure 4. Average root mean square error and standard deviation for 10 sets unseen B1+ maps for full optimal control solution, propagated neural network, and lastly drawing a set of parameters from the training set.

Figure 5: Example inversion performance for a central axial slice. Left – optimal control solution, right – propagated neural network solution.

Proc. Intl. Soc. Mag. Reson. Med. 26 (2018)
3388