Yiming Dong1, Malte Riedel2, Kirsten Koolstra3, Matthias J.P. van Osch1, and Peter Börnert1,4
1C.J. Gorter Center for High Field MRI, Department of Radiology, LUMC, Leiden, Netherlands, 2University and ETH Zurich, Zurich, Switzerland, 3Division of Image Processing, Department of Radiology, LUMC, Leiden, Netherlands, 4Philips Research, Hamburg, Germany
Synopsis
Multi-shot EPI readout-approaches provide
high spatial resolution at reduced geometric distortions and improved SNR in
diffusion weighted imaging (DWI). As a specific challenge, multi-shot
acquisition data require corrections for motion-induced, shot-specific phase
errors, e.g. using additional navigator signals or appropriate self-navigation.
Furthermore, proper fat-suppression is challenging in DWI, especially at B0
critical regions, making the use of chemical-shift encoding interesting. Therefore,
an iterative, model-based reconstruction algorithm with self-navigation and
water/fat decomposition, is proposed in this work. In-vivo examples in the leg
and head-neck regions demonstrate improved water/fat separation as compared to
acquisition-navigator approaches, while measurement times can be shortened.
Introduction
Fat is a confounding factor for EPI-based
diffusion-weighted imaging (DWI)1 due to the large chemical-shift
effect. To overcome the imperfections of conventional fat-suppression
techniques, chemical-shift encoding2,3
has been recently proposed4-6 to handle even multipeak fat spectra
in EPI5,6. Multi-shot EPI has gained growing popularity7,8
in DWI to reduce geometric distortion, making motion-induced shot-to-shot phase
errors correction via extra-navigated7,8 or self-navigated9-11
approaches necessary. However, when combined with chemical-shift encoding, the
presence of shifted fat in the navigator signal can impair image reconstruction
and degrade the quality of final water images. To circumvent such artefacts, we
propose an extended model-based
self-navigated water/fat decomposition resolved EPI (MSDE) image reconstruction
algorithm to jointly estimate water and fat while correcting
for the motion-induced shot-to-shot phase variations. The adverse effects of
the shifted fat are successfully mitigated, and no extra navigator8 signal
is required. Methods
The DW
signal model $$$s_{n,l,j}$$$ for
a k-space sample $$$k_{t}$$$ at the $$$n$$$-th chemical-shift
encoding point $$${\Delta}{{TE}_{n}}$$$,
shot $$$l$$$ and coil $$$j$$$ can be written as:$$s_{n,l,j}(t)=\int\left[c_{j}(r)\rho_{w}(r)+\sum_{m=1}^{M}\alpha_{m}c_{j}(r)\rho_{f}(r)e^{i\psi_{f,m}\left({\Delta}{{TE}_{n}}+t\right)}\right]e^{i2\pi\psi_{B}(r){\Delta}{{TE}_{n}}}e^{i\phi_{n,l}(r)}e^{-ik_{t}r}dr\tag{1}$$where $$$\rho_{w}$$$ and $$$\rho_{f}$$$ denote the complex-valued water/fat
components, $$$c_{j}$$$ the sensitivities,
$$$\alpha_{m}$$$ and $$$\psi_{f,m}$$$ the relative amplitude and chemical-shift for
each peak $$$m$$$ of the M-peak fat model, and $$$r$$$ the
spatial position. $$$\psi_{B}$$$ is the B0 inhomogeneity and $$$\phi_{n,l}$$$ the motion-induced phase, which are
modulated in image-space avoiding the computational burden12,13 imposed by
equivalent k-space convolutions. The extended
model-based water/fat separation can be solved with the conjugate gradient
method (CG), by minimizing:$$\left\{P_{w},P_{f}\right\}=\underset{P_{w},P_{f}\in\mathbb{C}^{Q}}{\operatorname{argmin}}\|\hat{A}X-S\|_{2}^{2}\tag{2}$$where
$$$Q$$$ is the number of voxels, $$$\hat{A}$$$ the coefficient matrix, $$$X=\left[P_{w},P_{f}\right]^{T}=\left[\rho_{w}^{1},\ldots,\rho_{w}^{Q},\rho_{f}^{1},\ldots,\rho_{f}^{Q}\right]^{T}$$$ the water/fat
images, and $$$S$$$ the joint vectorized
representation of all signals for $$$N$$$ chemical-shift encoding points, $$$L$$$ shots, and $$$J$$$ coils. The sequence
and general reconstruction pipeline are illustrated in Figure 1. It is the aim
to fully leverage all data sampled in a usual DWI scan. Thus, from
chemical-shift encoded non-DWI measurements, a B0 map, and water and
fat threshold-based masks can be derived using an image-based water/fat
decomposition approach for EPI (IDE)6. Furthermore, those non-DWI data
are used to estimate coil-sensitivity maps (CSM) that match the EPI scan data
conditions (geometric distortion). This is done by 1) using water-fat-JSENSE14,
or 2) through ESPIRiT15 by performing water/fat separation for data
acquired by each coil individually (with the estimated B0 map from previous
step) and estimating the merged water/fat (position-corrected) CSM.
For the diffusion measurements, a Gauss-Newton
solver is implemented to jointly estimate water, fat and shot-to-shot phase
maps. Using first-order Taylor expansion, the phase term error can be approximated
as $$$e^{i\Delta\phi_{n,l}(\boldsymbol{r})}{\approx}1+i\Delta\phi_{n,l}(\boldsymbol{r})$$$ and updated for
the next iteration. The number of iterations is empirically chosen to be 10. The unknown vector $$${\Delta}Y$$$
can be determined
by minimizing,$$\left\{{\Delta}P_{w},{\Delta}P_{f},{\Delta}\Phi_{1,1},\ldots,\Delta\Phi_{N,1},\ldots,\Delta\Phi_{N,L}\right\}=\underset{\Delta\Phi_{n,l}\in\mathbb{R}^{Q}\atop{\Delta}P_{w},{\Delta}P_{f}\in\mathbb{C}^{Q}}{\operatorname{argmin}}\|\hat{B}{\Delta}Y-{\Delta}S\|_{2}^{2}\tag{3}$$where
$$$\hat{B}$$$ is the coefficient matrix of the Gauss-Newton
system, $$$\Delta\Phi_{n, l}=\left[\Delta\phi_{n,l}^{1},\ldots,\Delta\phi_{n,l}^{Q}\right]^{T}$$$ for $$$n=1,\ldots,N;l=1,\ldots,L$$$, and $$$\Delta{S}=S-\hat{A}\bar{X}$$$ with the current estimated $$$\bar{X}$$$. The pre-calculated water/fat masks are applied to
the pre-estimated CSM to stabilize the estimation. To enforce smoothness of the
estimated phase maps, a 2D triangular window14 (width set empirically
to 5/6 of the matrix size) is applied in k-space for each Gauss-Newton
iteration.
Experiments
were conducted in head-neck regions and in the
lower leg (4
subjects, 3T, Philips, Best, The Netherlands), using a
spin-echo DW segmented EPI sequence with three b-values (0, 200, 400 s/mm2) or (0,
300, 600 s/mm2) sampling 4 or 6 interleaves at TE = 64 or 59 ms using 16-channel head-neck or 8-channel
knee coil with TR=2000 ms at resolution: 1.4×1.5×4 mm3. The three $$${\Delta}{TE}$$$ were chosen as 0.2/ 1.0/ 1.8 ms with respect to the spin echo. For comparison, an extra
2D-navigator8 was acquired for each diffusion shot. A multi-peak fat
model6 was used for all reconstructions.Results
Figure
2 shows a DWI data set reconstructed using the proposed MSDE approach with the CSM
obtained from SENSE pre-scan, ESPIRIT, and water-fat-JSENSE, respectively. The
two approaches using self-calibrated CSM show improved water images compared
to the one with the pre-scan. Figure 3 shows results of one subject’s leg, comparing IDE, the extended model-based
water/fat separation with extra navigators, and the proposed self-navigated (MSDE).
The artefacts shown in the water/ADC maps of the first two methods can be eliminated
by using self-navigation. Figure 4 shows estimated phase maps from MSDE at one $$${\Delta}{TE}$$$ and the phase/magnitude of the extra navigators
which contain shifted fat signal for comparison. Figure 5 shows the performance
of the three approaches in the head-neck region. The examples show that the MSDE
can avoid signal cancellations in the extra-navigated results.Discussion and conclusion
The
proposed MSDE algorithm provides more reliable water/fat separation for DWI
compared to IDE. This is guaranteed by (1) the model-based reconstruction with
fat off-resonance modulation in k-space, (2) the reduction of the spatial
mismatch between CSM and EPI data, via integrated CSM estimation, (3)
self-navigation to avoid measuring extra navigators which prolong acquisition
times, suffer from poor SNR (acquired at TE > 100ms) and contain shifted fat
signal, and (4) chemical-shift encoding, as an intelligent way of doing signal
averaging, providing more data that help to better condition the inverse
problem. This also supports the self-navigation to deal with the increased
g-factor effects at large shots number.Acknowledgements
The authors would like to acknowledge NWO-TTW (HTSM-17104).References
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