Oriana Vanesa Arsenov1, Karin Shmueli1, and Anita Karsa1
1Medical Physics and Biomedical Engineering, University College London, London, United Kingdom
Synopsis
Current techniques for background
field removal (BGFR), essential for quantitative susceptibility mapping, leave residual
background fields and inaccuracies near air-tissue
interfaces.
We propose a new deep learning
method aiming for robust brain BGFR: we trained a 3D U-net with realistic
simulated and in-vivo data augmented with spatial deformations.
The network trained on
synthetic data predicts accurate local fields when tested on synthetic data,
(median RMSE = 49.5%), but is less accurate when tested on in-vivo
data. The network trained and tested on in-vivo data performs better,
suggesting our synthetic set did
not fully capture the complexity found in vivo.
Introduction
Quantitative
susceptibility mapping (QSM) uses phase images to calculate the underlying
tissue magnetic susceptibility and background field removal (BGFR) is a crucial
step in the QSM pipeline1. The total field in the brain (Btot)
is created by susceptibility sources located both inside (inducing the “local”
field, Bint), and outside the brain (inducing the background field, Bext). BGFR aims
to eliminate these background fields to obtain Bint from which the
susceptibility is calculated. Existing BGFR techniques2 are
based on assumptions (e.g. no harmonic Bint)
which are often violated, leading to residual Bext and inaccuracies near air-tissue interfaces.
We trained a deep learning network using
realistic simulated and in-vivo data augmented using random spatial
deformations, aiming to perform accurate and robust BGFR in the brain. Methods
An adapted convolutional neural network (CNN), a 3D U-net created for QSM
reconstruction3 (Figure 1), was trained using a synthetic dataset (Model 1) and
an in-vivo dataset (Model 2).
Model 1: Realistic field variations were simulated
in an anthropomorphic head-and-neck phantom4. To mimic different
head shapes, random spatial deformations were performed by applying B-Spline
transformations with control point spacing=8 voxels and amplitude range=6
voxels and again with spacing=64 voxels, amplitude ranges=20 voxels, using a Matlab toolkit for nonrigid image registration5. Realistic
susceptibility values randomly varying between ±0.2 ppm were assigned to nine
different brain structures. Baseline tissue and air susceptibilities were set
to -9.4 ppm and 0 ppm, respectively. Btot and Bint pairs
were calculated using the simulated reference scan method4 (Figure
2): 1. Btot were computed from the
susceptibility maps (all sources) using the forward model6, 2. Bext
were calculated6 from maps containing only the susceptibility
difference between tissue and air (outside sources) i.e. without any
susceptibility structures in the brain, and 3. Bint=Btot-Bext. Noise
normally distributed between ±0.02 ppm was added to the Btot input maps, while Bint ground truth maps were kept noise-free.
For training and testing, 90 and 10 pairs,
respectively, of input Btot
maps and target Bint
maps were used. The root-mean-square errors (RMSE) between the ground truth and
predicted Bint for all ten test images were calculated and the median value was used to assess
model accuracy.
Model 2: In-vivo
head-and-neck images were acquired at 3T in 8 healthy volunteers7 with a 3D GRE sequence, 16-channel receive coil, 1.25mm isotropic voxels, 4
echoes, TE1=ΔTE/TR=4.61/22ms, SENSE R2 and flip-angle=12°. Susceptibility maps were calculated7 using nonlinear field fitting8,9, Laplacian phase unwrapping10,
BGFR with projection onto dipole fields (PDF)11, and iterative
Tikhonov regularisation (α = 0.11). To increase the training sample, similar
to the synthetic images, the susceptibility maps were randomly deformed5 and the susceptibility values of 13 regions of interest (ROI, automatically
segmented using FSL FIRST12) were varied by adding a random constant
susceptibility between ±0.2 ppm to
each ROI. Here, the baseline tissue susceptibility was set to -8 ppm and
a random variation between ±0.1 ppm
was added to realistically augment Btot. For training, a set
of 100 images was generated and downsampled by a factor of 2 to reduce
computational requirements. The CNN
architecture and hyperparameters (batch size=3, no. of epochs=1000) were the same as for Model 1 (Figure 1).
Models 1 and 2 were tested on Btot maps calculated
(using nonlinear field fitting and Laplacian phase unwrapping) from brain
images acquired at 3T4 in five healthy female volunteers using a 3D
GRE sequence, 32-channel receive coil, 1mm isotropic voxels, 5 echoes,
TE1/ΔTE/TR = 3/5.4/29ms, SENSE R1x2x1.5 and flip-angle=20°.
Both models' performance was compared to that of PDF.Results
For Model 1, the median RMSE across
subjects was 49.5%. Figure 3 shows an example of the ground truth
and predicted Bint together
with their difference. The results of testing Model
1 in vivo are presented in Figure 4. An example of the performance of Model 2 is shown in Figure 5.Discussion
When tested on synthetic data, the network
trained on synthetic data, Model 1, predicts accurate Bint, close to the ground truth, with reduced
artifacts near brain edges (Figure 3) compared to the results of existing
techniques2. However, this network’s accuracy was much lower when
tested in vivo (Figure 4). Bint
were underestimated by an order of magnitude and a checkered field pattern was
present probably because the synthetic training set did not fully capture the complexity of in-vivo data.
Model 2, trained on in-vivo images, performed
better than Model 1 when tested on in-vivo images. Figure 5 shows that Bint were still slightly
underestimated compared with PDF, particularly at susceptibility
interfaces/edges. We plan to use a larger training sample, consisting of both
synthetic and in-vivo images with a wider range of resolutions, to minimise
these differences.Conclusion
We
designed a new deep learning method for BGFR by using random spatial deformations
to simulate realistic total and background fields in a numerical phantom and to
augment total field maps in vivo, and using these two datasets to train a CNN.
The network trained on synthetic images performs significantly better when
tested on synthetic data than on in-vivo volunteer data. Training the CNN on
augmented in-vivo images increased its accuracy for predicting local field maps
for in-vivo images.Acknowledgements
Dr Karin Shmueli is supported by European Research Council Consolidator Grant DiSCo MRI SFN 770939.References
1. E.
Haacke, S. Liu, S. Buch, W. Zheng, D. Wu and Y. Ye. Quantitative susceptibility
mapping: current status and future directions. Magnetic Resonance
Imaging, vol. 33, no. 1, pp. 1-25, 2015. Available:
10.1016/j.mri.2014.09.004.
2. F.
Schweser, S. Robinson, L. de Rochefort, W. Li and K. Bredies. An illustrated
comparison of processing methods for phase MRI and QSM: removal of background
field contributions from sources outside the region of interest. NMR in
Biomedicine, vol. 30, no. 4, p. e3604, 2016. Available: 10.1002/nbm.3604.
3. S. Bollmann. Deep learning QSM tutorial OHBM. Colab.research.google.com,
2018. [Online]. Available:
https://colab.research.google.com/github/brainhack101/IntroDL/blob/master/notebooks/2019/Bollman/Steffen_Bollman_Deep_learning_QSM_tutorial_OHBM.ipynb. [Accessed:
13- Jan- 2020].
4. Karsa,
A., Punwani, S. and Shmueli, K. The effect of low resolution and coverage on
the accuracy of susceptibility mapping. Magnetic Resonance in Medicine,
81(3), pp.1833-1848, 2018.
5.
Dirk-Jan Kroon. B-spline Grid, Image and Point based Registration, 2020.
[Online]. Available:
https://www.mathworks.com/matlabcentral/fileexchange/20057-b-spline-grid-image-and-point-based-registration),
MATLAB Central File Exchange. Retrieved December 14, 2020.
6. Marques, J. and Bowtell, R. Application of a Fourier-based method for
rapid calculation of field inhomogeneity due to spatial variation of magnetic
susceptibility. Concepts in Magnetic Resonance Part B: Magnetic
Resonance Engineering, 25B(1), pp.65-78, 2005.
7. Karsa, A., Punwani, S., &
Shmueli, K. An optimized and highly repeatable MRI acquisition and processing
pipeline for quantitative susceptibility mapping in the head‐and‐neck
region. Magnetic Resonance in Medicine, 84(6),
3206-3222, 2020.
8.
Liu T, Wisnieff C, Lou M, Chen W, Spincemaille P, Wang Y. Nonlinear
formulation of the magnetic field to source relationship for robust
quantitative susceptibility mapping. Magnetic Resonance in Medicine, 69(2), 467-476, 2013.
9. Cornell MRL. MEDI toolbox.
[Online]. Available: http://weill.cornell.edu/mri/pages/qsm.html.
10. Biondetti E, Thomas DL, Shmueli K.
Application of Laplacian-based methods to multi-echo phase data for accurate
susceptibility mapping. In: Proceedings of ISMRM 24th Annual Meeting,
Singapore; 2016:1547.
11. Liu, Tian, et al. A novel background
field removal method for MRI using projection onto dipole fields. NMR
in Biomedicine, 24(9), 1129-1136, 2011.
12. Patenaude, B., Smith, S. M., Kennedy,
D. N., & Jenkinson, M. A Bayesian model of shape and appearance for
subcortical brain segmentation. Neuroimage, 56(3),
907-922, 2011.