Yannick Brackenier1, Nan Wang1, Congyu Liao1, Xiaozhi Cao1, Sophie Schauman1, Mahmut Yurt2, Lucilio Cordero-Grande3, Shaihan J Malik4,5, Adam Kerr2,6, Joseph V Hajnal4,5, and Kawin Setsompop1,2
1Department of Radiology, Stanford University, Stanford, CA, United States, 2Department of Electrical Engineering, Stanford University, Stanford, CA, United States, 3Biomedical Image Technologies, ETSI Telecomunicación, Universidad Politécnica de Madrid and CIBER-BNN, Madrid, Spain, 4Biomedical Engineering Department, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 5Centre for the Developing Brain, School of Biomedical Engineering and Imaging Sciences, King's College London, London, United Kingdom, 6Cognitive and Neurobiological Imaging (CNI), Stanford University, Stanford, CA, United States
Synopsis
Keywords: Motion Correction, Brain
‘Scout-based’ navigators exploit correlations between navigator data and a low-resolution multi-coil pre-scan data (scout) to
effectively estimate either motion or B
0-perturbations. Usually,
scout data has a fixed contrast, limiting their usage in estimating motion within
echo-trains where contrast changes from one readout to the next (e.g. MPRAGE).
Furthermore, combined motion and B
0-perturbation estimation from
rapid navigators has yet to be achieved. In this work, we propose a
quantitative scout (Q-SCOUT) to ‘time-resolve’ navigator contrast, along with a
rapid SPINS-navigator (few ms). Q-SCOUT and rapid navigator data are used in
our QUEEN method to enable
within-echo-train motion and B
0-perturbation
estimation.
Introduction
MRI is susceptible to motion and B0-inhomogeneity perturbations[1]. Navigator-based techniques have been developed to estimate and correct for
these, including methods that utilize a pre-scan to guide motion/B0 estimation.
Within this class, the cloverleaf and spherical navigators[2-3] utilize tailored k-space trajectories to sensitize signals to rigid motion. FID multi-coil
navigators [4] have been augmented with a low-resolution pre-scan ‘scout’ image
to enable accurate motion[5] or B0-perturbation[6]
estimation. Similarly, the “SAMER+guidance-lines”[7] approach utilizes a
single-contrast scout along with 4 lines of k-space acquisition from an echo-train
to achieve accurate inter-echo-train motion estimation. In this work, we
propose “Quantitatively-Enhanced parameter Estimation from Navigators (QUEEN)”,
to provide robust combined motion and B0-perturbation estimation
for both inter- and within-echo-train correction by using a
time-resolved multi-contrast scout. A short navigator of a few ms was developed
and can be flexibly inserted in most sequences. QUEEN’s novel components include i) a ‘quantitative’ scout scan (Q-SCOUT), ii) time-resolved motion and B0
estimation and iii) a tailored SPINS navigator[8].Methods
Q-SCOUT:
This work extends the concept of a single-contrast scout to
a time-resolved quantitative scout (Q-SCOUT) that models the time-varying navigator
signal (Fig1) to enable navigator usage in almost any sequence and/or timing. To correct for
brain motion and B0-perturbation ($$$\delta \textbf{B}_0$$$), a low-resolution Q-SCOUT is
sufficient for which fast quantitative imaging sequences such as MRF and EPTI[9,10]
can be used. Fig1 showcases a 7s MRF acquisition to obtain whole-brain PD, T1,
T2 and coil sensitivity information at 4mm isotropic resolution.
QUEEN:
Whereas the Q-SCOUT predicts the time-varying navigator signal $$$\textbf{Q}_s(t)$$$ (Fig2), QUEEN refers to the estimation of motion and $$$\delta \textbf{B}_0$$$ parameters. Navigator k-space is
modeled as a time-segmented signal:
$$
\textbf{y}_n =
\textbf{F}_n\textbf{ST}(\textbf{z})\textbf{P}_n(\delta \textbf{B}_0)\textbf{Q}_{s_n}\quad\quad(1)
$$
for time-segments $$$n=1:N$$$, where $$$\textbf{F}_n$$$ is the
segment-dependent non-uniform Fourier transform, $$$\textbf{P}_n$$$ the induced
phase $$$e^{2\pi \delta \textbf{B}_0t_n}$$$ and $$$\textbf{Q}_{s_n}$$$ the Q-SCOUT-predicted contrast at time $$$t_n$$$. $$$\textbf{T}(\textbf{z})$$$ represents the rigid motion operator (with rigid motion parameters $$$\textbf{z}$$$) and $$$\textbf{S}$$$ contains the coil sensitivities.
We model $$$\delta \textbf{B}_0$$$
using a
set of 2nd-order solid harmonics (SH) [11] ($$$\delta \textbf{B}_0=\textbf{Bc}$$$ with SH
basis $$$\textbf{B}$$$ and coefficients $$$\textbf{c}$$$) and
iteratively estimate motion and $$$\textbf{c}$$$ using the Levenberg-Marquardt algorithm:
$$
\textbf{z}^{i+1}=argmin_\textbf{z}\sum_{n=1}^{N}||
\textbf{F}_n\textbf{ST}(\textbf{z})\textbf{P}_n(
\textbf{c}^{i})\textbf{Q}_{s_n}-\textbf{y}_n||^2_2\quad\quad(2)
\\\textbf{c}^{i+1}=argmin_\textbf{c}\sum_{n=1}^{N}||
\textbf{F}_n\textbf{ST}(\textbf{z}^{i+1})\textbf{P}_n(
\textbf{c})\textbf{Q}_{s_n}-\textbf{y}_n||^2_2\quad\quad(3)
$$
SPINS:
The SPINS trajectory, originally designed for B1+-mitigated
RF excitation, is used here due to its rapid acquisition and sensitivity to
rigid motion and B0 inhomogeneity: arc-sampling at multiple radii sensitizes
signal to rotation and translation whilst sampling the k-space origin at
start and end results in B0 sensitivity. Acquisition time was minimized
using gradient trajectory optimization[12] (Fig1).
Simulations:
Simulation 1 compares the FID and SPINS navigator
trajectory when simulating ‘within-TR’ navigator signal for an SPGR sequence (Fig2):
baseline B0- and R2*-resolved signal is simulated in the presence of
motion and $$$\delta \textbf{B}_0$$$. Motion
is QUEEN-estimated by either ignoring $$$\delta \textbf{B}_0$$$
(“motion-only”)
or joint optimization (“motion-$$$\delta \textbf{B}_0$$$
”). Simulation 2 simulates
‘within-echo-train’ navigator signal for MPRAGE at different inversion times
(TI) (Fig3).
Motion is estimated using either the correct TI (Q-SCOUT+QUEEN) or a fixed TI (fixed-SCOUT+non-QUEEN).
Other effects on the signal (e.g. readout RF excitations) are ignored for simplicity but can be incorporated. B0 can be ignored since MPRAGE usually uses short TEs,
making the FID navigator preferable due to its arbitrary duration. By
acquiring a 1ms FID navigator every 169ms, this simulation mimics high-temporal resolution within-echo-train motion estimation with minimal efficiency loss (0.5%).
In-vivo:
The ‘within-TR’ QUEEN was tested on a healthy volunteer by
implementing the proposed SPINS in a multi-echo GRE (Fig5). Q-SCOUT data was
generated at 4x4x4mm3 by retrospectively under-sampling the image
acquisition and fitting B0 and R2* maps from multi-echo images. Gradient
trajectories were measured using a Skope field camera[13]. Data
was acquired in 1) a reference pose and 2) a different pose whilst placing the
arms close to the head to induce B0 variation. QUEEN was compared to
the ground truth, obtained by registering reconstructed images and B0
maps. ROVir coil compression[14] was used to suppress signal from regions of non-rigid
neck motion.Results and discussion
Results
for simulation 1 are shown in Fig3, where coupling between motion and $$$\delta \textbf{B}_0$$$
estimation is
observed (3.A -B). Improved estimation is obtained for the proposed “motion-$$$\delta \textbf{B}_0$$$
” QUEEN
optimization. Furthermore, SPINS outperform the FID trajectory in the presence of
$$$\delta \textbf{B}_0$$$. Results for simulation 2 (Fig4) show
that the time-resolved Q-SCOUT drastically improves the
QUEEN motion estimation for TIs away from the fixed-SCOUT. Even with the
Q-SCOUT, slight sensitivity of parameter estimation to contrast is observed (4.B).
In-vivo results (Fig5) confirm improved motion estimation for the “motion-$$$\delta \textbf{B}_0$$$” QUEEN, although with
reduced accuracy compared to simulations. Observed systematic signal inconsistencies
(not shown) are hypothesized to be the cause.Conclusion
We have proposed a quantitative scout (Q-SCOUT) to
predict time-resolved navigator contrast for enhanced motion and B0-perturbation
estimation (QUEEN). A rapid
navigator was developed for this purpose and can be flexibly inserted in most
sequences. Simulations show the potential of Q-SCOUT+QUEEN
to achieve improved motion estimates, especially in the presence of B0-perturbations. This
was confirmed in-vivo, although model imperfections limit the achieved accuracy.
Future work will investigate these model imperfections and translate the proposed
approach to in-vivo within-echo-train motion correction.
Acknowledgements
This work was partly funded by
the King’s College London & Imperial College London EPSRC Centre for
Doctoral Training in Medical Imaging [EP/S022104/1].References
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