Synopsis
A novel
compartmental low rank algorithm and data acquisition method for high
resolution MR spectroscopic imaging without the use of any lipid suppression
methods is introduced. The field inhomogeneity compensated data is modeled as
the sum of a lipid dataset and a metabolite dataset using the spatial
compartmental information obtained from the water reference data. These
datasets are modelled to be low-rank subspaces and are assumed to be mutually
orthogonal. The high resolution spiral acquisition method achieves in plane resolution of upto 1.8x1.8 mm2 in 7.2 mins. Recovery from these measurements
is posed as a low rank recovery problem. Experiments on in-vivo data
demonstrates comparable results for both lipid suppressed and lipid unsuppressed
data.Introduction
Spectral leakage from extracranial lipids, whose
concentrations are several folds higher than that of the metabolites, causes
severe artifacts in MR spectroscopic imaging (MRSI). The
effects of spectral leakage are even more aggravated at low resolution due to
truncation artifacts. Several methods used for lipid suppression like outer
volume suppression, inversion recovery, selective excitation, long echo times
etc[1,2,3], result either in signal loss or in partial brain coverage. Improved
k-space coverage reduces lipid leakage [4], but at the cost of deteriorated
metabolite SNR and increased scan time.
In this work we
introduce a novel compartmental low rank algorithm for high resolution MR
spectroscopic reconstruction for lipid unsuppressed data. We use the spiral
data acquisition scheme introduced in [5], to achieve high spatial resolution
MRSI, in a reasonable scan time and with minimal SNR loss. We model the field
inhomogeneity compensated data as the sum of two low-rank subspaces for
metabolites and lipids which are mutually orthogonal.Experimental results demonstrate the performance of the proposed algorithm with and without the use of lipid suppression methods.
Methods
Variable density multi-shot spirals were used to obtain matrix
sixe of 128x128 with the center k-space region of 32x32 averaged 12 times. This
achieves an in-plane spatial resolution of upto 1.8x1.8 mm2 at a
scan time of 7.2 mins/slice with TR=1.5 ms. A separate water reference data is
acquired in 2.4 mins/slice(TR=0.5 secs) and was processed using [6] to obtain high
resolution B0 map and lipid and brain masks that characterize
the spatial compartments.
The field inhomogeneity corrected spatio-temporal data is
modeled as the sum of low-rank compartments belonging to metabolites ($$$ X_{M} $$$)
and lipids ($$$ X_{L} $$$) respectively;
$$$ X(r,t) =
X_{M}(r,t)+X_{L}(r,t) $$$ . These
compartments are assumed to be low rank and their spatial support is given by
the metabolite and lipid masks. Using a single low-rank subspace to model the
entire dataset is not effective because, the massive dynamic range between
lipids and metabolites results in the subspace being dominated by the lipid basis
functions. We exploit the orthogonality between metabolites and lipids as
established in [7] to minimize lipid leakage artifacts. This enables us to
recover the subspaces without imposing any prior knowledge of the spectral
support. The recovery is formulated as the optimization problem,
$$
f(X) = \arg\min_{X_{M},X_{L}}
\|\mathcal{A}X-b\|+\lambda_{1}\|X_{M}\|_{p}+\lambda_{2}\|X_{L}\|_{p} $$
$$ \text{for} \ p \leq 1 \ \text{such that} \ X_{M} \perp X_{L} $$
where
$$$\mathcal{A}$$$ is the forward
model accounting for the non-uniform Fourier transform, field inhomogeneity,
and coil sensitivity encoding and $$$b$$$ is the measured data. Water is removed as a pre-processing step using
HSVD [8]. Equation (2) is solved using iterative reweighted least square
algorithm [9].
This work has some conceptual similarities to [10,11]. However
what distinguishes the proposed method is the absence of specialized data
acquisition and processing steps for estimating the metabolite and lipid basis
functions that explicitly account for the spectral support. The subspaces for
metabolites and lipids are automatically estimated from the measured data.
Hence the proposed method is not sensitive to line broadening of lipids and metabolites;
and robust to deviation from known spectral location which may occur in practical
applications with large field variations near the skull. Also in addition these
methods employ outer volume suppression or long echo times.
Results
Data is collected on
a single axial slice of FOV
xy = 24 cm,slice thickness of 1cm at TR/TE = 1500/55
ms. The dataset is once collected without any lipid suppression method and once
with 8 OVS bands(lipid suppressed). The datasets are reconstructed on a 96x96 grid size using a
standard pipeline of inverse Fourier transform & field inhomogeneity
compensation(IFFT Reconstruction) and the proposed method. Fig(1) compares the
peak integral NAA maps for both the datasets using both the methods. Maps
obtained from IFFT reconstruction shows severe lipid leakage even with the use
of OVS bands , whereas the proposed method retains high resolution details and
eliminates lipid leakage artifacts. Fig(2) shows the spectra for both the
datasets at the pixels marked in the reference image. Spectra from IFFT
reconstruction are plotted in blue and the ones from the proposed method in
red. Spectra from IFFT reconstruction show lipid leakage and are noisy. The
proposed method recovers denoised spectra and lipid leakage is removed. The
reconstructed lineshape for both the lipid suppressed and unsuppressed data are
comparable.
Conclusion
We introduced a novel
low-rank based reconstruction method for high resolution MRSI which is robust
to lipid leakage even while recovering from lipid unsuppressed data. We
demonstrate comparable reconstructions for lipid suppressed and unsuppressed
data using the proposed method.
Acknowledgements
Grant sponsor:American Cancer Society; Grant number:RSG CCE-121672References
[1] Chu, A., Alger, J. R., Moore, G. J., & Posse, S. (2003). Proton echo-planar spectroscopic imaging with highly effective outer volume suppression using combined presaturation and spatially selective echo dephasing. Magnetic resonance in medicine, 49(5), 817-821.
[2] Bydder, G. M., & Young, I. R. (1985). MR imaging: clinical use of the inversion recovery sequence. Journal of computer assisted tomography, 9(4), 659-675.
[3] Bottomley, P. A. (1987). Spatial localization in NMR spectroscopy in vivo. Annals of the New York Academy of Sciences, 508(1), 333-348.
[4] Ebel, A., & Maudsley, A. A. (2003). Improved spectral quality for 3D MR spectroscopic imaging using a high spatial resolution acquisition strategy. Magnetic resonance imaging, 21(2), 113-120.
[5] Bhattacharya I. , Jacob M.(2015). High Resolution 1H MRSI without lipid suppression at short echo times using variable density spirals;in Proc of ISMRM 2015, #2017.
[6] Cui, C., Wu, X., Newell, J. D., & Jacob, M. (2015). Fat water decomposition using globally optimal surface estimation (GOOSE) algorithm. Magnetic Resonance in Medicine, 73(3), 1289-1299.
[7] Bilgic, B., Gagoski, B., Kok, T., & Adalsteinsson, E. (2013). Lipid suppression in CSI with spatial priors and highly undersampled peripheral k-space. Magnetic Resonance in Medicine, 69(6), 1501-1511.
[8] Barkhuijsen, H., De Beer, R., & Van Ormondt, D. (1987). Improved algorithm for noniterative time-domain model fitting to exponentially damped magnetic resonance signals. Journal of Magnetic Resonance (1969), 73(3), 553-557.
[9] Fornasier, M., Rauhut, H., & Ward, R. (2011). Low-rank matrix recovery via iteratively reweighted least squares minimization. SIAM Journal on Optimization, 21(4), 1614-1640.
[10] Lam, F., & Liang, Z. P. (2014). A subspace approach to high-resolution spectroscopic imaging. Magnetic Resonance in Medicine, 71(4), 1349-1357.
[11] Ma, C., Lam, F., Johnson, C. L., & Liang, Z. P. (2015). Removal of nuisance signals from limited and sparse 1H MRSI data using a union-of-subspaces model. Magnetic Resonance in Medicine.