Julia Traechtler1, Valery Vishnevskiy1, Maximilian Fuetterer1, Andreas Dounas1, and Sebastian Kozerke1
1Institute for Biomedical Engineering, University and ETH Zurich, Zurich, Switzerland
Synopsis
An advanced signal model-based reconstruction jointly estimating image
and field map from multi-echo, multi-coil acquisition of hyperpolarized
metabolic data was developed and validated using synthetic and in-vivo data. Relative
to standard multi-echo reconstruction methods, reconstruction accuracy improved
by up to 30% for synthetic data considering
realistic noise levels and field map gradients. Geometric distortion correction
resulted in less than 20% error. For in-vivo data, the average improvement was
15%. Depending on the direction of the field gradients present, multi-coil
reconstruction was found to be beneficial for addressing signal folding issues.
Introduction
Hyperpolarized 13C magnetic resonance imaging has shown
potential for imaging metabolism of the in-vivo human heart1.
Multi-echo acquisition2 combined with reconstruction techniques that
deconvolve signal contributions of individual metabolites based on their known chemical shift3 have been proposed for
hyperpolarized 13C MRI4. However, multi-echo
reconstruction is sensitive to B0 induced phase offsets and
therefore more advanced reconstruction techniques are required5,6. In
the present work, a model-based reconstruction jointly estimating image and
field map from multi-echo data is proposed and validated using synthetic and
in-vivo data.Methods
An advanced model-based reconstruction of multi-echo,
multi-coil hyperpolarized metabolic data is presented (cf. Fig-1). The signal
model accounts for chemical shift $$$f(m)$$$ dependent spatial shifts of metabolite $$$m$$$ as well as distortions induced by varying in-plane
off-resonances $$$B_0$$$. Sampling along a trajectory $$$\vec{k}$$$ at time points $$$t_s$$$ and considering weighting terms due to
coil sensitivities $$$C(\vec{x})$$$ as well as $$$T_1$$$, $$$T_2^*$$$ relaxation, and spectral-spatial excitation $$$\alpha(\vec{x})$$$, yields the signal:
$$\underbrace{s(\vec{k},d,e)}_{\vec{s}}=\underbrace{\sum_{\vec{x}}e^{j\vec{k}\vec{x}}\sum_m{}e^{j2\pi{}f(m)t(e)}\cdot{}C(\vec{x})\cdot{}e^{-\frac{t_{Dyn}(d)}{T_1(m)}}\cdot{}e^{-\frac{t(e)}{T^{*}_2(\vec{x},m)}}\cdot{}\sin\left(\alpha(\vec{x},m)\right)\cdot{}\cos\left(\alpha(\vec{x},m)\right)^{e-1}}_{\mathbf{E}}\cdot{}\underbrace{e^{j2\pi{}B_0(\vec{x})t(e)}}_{\mathbf{\hat{B}_0}}\cdot{}\underbrace{\rho(\vec{x},d,m)}_{\vec{\rho}}+\eta~~~\text{[1]}$$
where $$$t=t_s+TE$$$ with $$$TE$$$ being the echo time of echo $$$e$$$, $$$\rho$$$ denoting the spatiotemporal object of dynamic $$$d$$$ and $$$\eta$$$ Gaussian noise.
Rewriting equation [1] in matrix notation $$$\vec{s}=\left(\mathbf{E}\cdot{}\mathbf{\hat{B}_0}\right)\vec{\rho}$$$, allows to
formulate image reconstruction as the following minimization problem optimizing
jointly for image and B0:
$$\underset{\vec{\rho},\mathbf{\hat{B}_0}}{\text{argmin}}{}\left|\left|\left(\mathbf{E}\cdot{}\mathbf{\hat{B}_0}\right){}\vec{\rho}-\vec{s}\right|\right|_2^2+\lambda_{\rho}|\nabla_x\vec{\rho}|_1+\lambda_{\hat{B}_0}|\nabla_x\mathbf{\hat{B}_0}|_1$$
with $$$\lambda_{\rho}$$$, $$$\lambda_{\hat{B_0}}$$$ being regularization parameters and $$$|\cdot|_1$$$, $$$||\cdot||_2$$$ denoting the L1- and L2-norm,
respectively.
The mathematical framework was implemented in Python using Tensorflow7
and executed on GPUs.
For the simulation study, echo-shift encoded data of metabolic
signals were generated using the simulation framework as described previously8.
An echo-planar imaging (EPI) trajectory (in-plane resolution=5x5mm2, FOV=85x85mm2) was used to generate synthetic k-space
data for different high-resolution (1x1mm2) B0
maps and coil sensitivities.
In-plane B0 maps with linear gradients, scaled by varying
beta factors (relative phase encoding bandwidth), were used to examine geometric
distortion and correction. Scaling by beta>0 stretches the object by a
factor of (1+beta) and beta<0 results in object compression with beta=-1
being a projection of the object.
Image reconstruction and off-resonance estimation accuracies
w.r.t. noise were analyzed for a single homogenous coil and constant beta=+0.2.
The effects of multi-coil encoding were tested for aliasing (beta=+0.5) using simulated
coil sensitivities generated using Biot-Savart’s law for one, two and four
coils, respectively.
In-vivo applicability was evaluated on synthetic data using six
coil sensitivity maps (estimated for reconstruction9) and three B0
map slices obtained from in-vivo data. Data was generated as the average of
three sub-slices to account for through-slice B0 variations. Imaging
parameters for the EPI trajectory were set according to in-vivo conditions: in-plane
resolution=5x5mm2, FOV=220x220mm2, slice thickness=20mm, lactate
signal-to-noise ratio (SNR) averaged over the myocardium of 15. Both EPI phase-encoding blip
directions left/right were analyzed.
Finally, the proposed method was tested on in-vivo data acquired in
three healthy pigs at 3T10 and compared to standard non-linear
conjugate gradient-based reconstruction without B0 correction. Measured
field maps (1H) served as reference for evaluating B0
estimation.
For the simulation studies, the pixel-wise normalized root-mean-square
error (nRMSE) between reconstructed image and ground truth object were
compared. For both, synthetic and in-vivo data, the DICE coefficient served as
quantification metric for the reconstructed images. B0 estimation
was evaluated based on the pixel-wise RMSE.
Regularization parameters were chosen according to RMSE using grid search.Results
Fig-2 shows reconstructed images and estimated B0 maps
for different in-plane B0 gradients beta=[+0.5,-0.5] corresponding
to a maximum B0 range of 236Hz at the carbon resonance frequency at
3T. Reconstruction accuracy in terms of RMSE and DICE decreases linearly with
increasing |beta| for reconstruction without B0 correction, whereas
the proposed reconstruction shows improved accuracy for beta=[+0.2,-0.1]. In
this range, distortion correction is feasible with less than 20% error.
Fig-3 illustrates the reconstruction for a fixed B0
gradient as function of SNR and number of coils, respectively. For
beta=+0.2, an increase in SNR to 12 significantly improves B0
estimation accuracy. In case of aliasing (beta=+0.5), increasing the number of
coils from one to two/four improves image and B0 RMSE by 4%/5% and 14%/23%, and DICE by 2%/4%, respectively.
Fig-4 shows reconstruction results for data simulated with in-vivo
B0 gradients for both EPI phase-encoding directions. For in-plane B0
gradients, the image RMSE of the proposed reconstruction is 14% lower compared
to the standard reconstruction. Through-plane B0 gradients, which are
not estimated, deteriorate reconstruction performance.
Fig-5 shows reconstructed in-vivo images with and without B0
correction. For all three examined in-vivo cases, the average improvement in DICE score
accounts for 15% for the proposed method compared to standard reconstruction
without B0 estimation.Discussion
Advanced multi-echo, multi-coil reconstruction allows for joint
estimation of image and field maps thereby addressing off-resonance induced geometrical
distortions and resonance separation issues. Given the relatively low spatial
resolution and SNR in hyperpolarized MRI, image and field map estimation
were found to be limited by SNR and field gradients. Based on accepting 20% reconstruction error, a lactate SNR>=12 and
a maximum field gradient covering 94Hz (beta=+0.2) is recommended.
Depending on the direction of the field gradients, multi-coil
reconstruction was shown to be beneficial in addressing signal folding issues.
In conclusion, joint image and field map estimation holds
promise to provide geometrically and chemically-shift consistent metabolic maps
in multi-echo
hyperpolarized MRI.Acknowledgements
No acknowledgement found.References
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