Changyu Sun1, Austin Robinson2, Christopher Schumann2, Daniel Weller1,3, Michael Salerno1,2,4, and Frederick Epstein1,4
1Biomedical Engineering, University of Virginia, Charlottesville, VA, United States, 2Medicine, University of Virginia, Charlottesville, VA, United States, 3Electrical and Computer Engineering, University of Virginia, Charlottesville, VA, United States, 4Radiology, University of Virginia, Charlottesville, VA, United States
Synopsis
Multiband (MB)
excitation and in-plane acceleration of first-pass perfusion imaging has the
potential to provide a high aggregate acceleration rate. Our recent
slice-SPIRiT work formulated MB reconstruction as a constrained optimization
problem that jointly uses in-plane and through-plane coil information and MB data
consistency. Here we extend these methods to develop k-t slice-SPARSE-SENSE and
k-t slice-L+S reconstruction models. First-pass perfusion data with MB=3 and
rate-2 k-t Poisson-disk undersampling were acquired in 6 patients. The
slice-L+S reconstruction showed sharper borders and greater contrast than
slice-SPARSE-SENSE and had better image quality scores as assessed by two
cardiologists.
Purpose
First-pass MRI is widely used to image
myocardial perfusion. While three slices are typically acquired1,
multiband (MB) and in-plane acceleration methods used together promise an
increased number of slices and better heart coverage. We recently developed a
MB reconstruction model that combines through-plane coil sensitivity, in-plane coil calibration consistency, and consistency with
acquired data for iterative joint estimation of all slices2. For MB excitation and in-plane acceleration,
here we further develop k-t slice-SPARSE-SENSE and slice-low-rank plus sparse3
(slice-L+S) reconstructions and apply them to first-pass imaging, including
comparisons of the two reconstructions. Theory
The k-t slice-L+S model utilizes
in-plane sensitivity maps and through-plane kernel calibration information for MB data consistency, and enforces temporal L+S3. The proposed slice-L+S reconstruction (Figure 1B) is expressed in Equation 1:
$$\mathop {\arg \min
}\limits_{L,S} {\left\| {H\left( {\begin{array}{*{20}{c}}
{{L_1} + {S_1}}\\
{{L_2} + {S_2}}\\
\vdots \\
{{L_{{N_s}}} + {S_{{N_s}}}}
\end{array}} \right) -
{y_{MB}}} \right\|^2} + {\lambda _L}{\left\| {\begin{array}{*{20}{c}}
{{L_1}}\\
{{L_2}}\\
\vdots \\
{{L_{{N_s}}}}
\end{array}} \right\|_*} +
{\lambda _s}{\left\| {T\left( {\begin{array}{*{20}{c}}
{{S_1}}\\
{{S_2}}\\
\vdots \\
{{S_{{N_s}}}}
\end{array}}
\right)} \right\|_1}, (1)$$
where the operator $$$H$$$
(Figure 1C) is defined as $$$H = PQE$$$, $$$N_s$$$ is the number of MB slices, $$$P_z$$$ is the CAIPIRINHA phase modulation matrix for
the $$$z^{th}$$$ slice, $$$F$$$ is the
fast Fourier transform, $$$E_z$$$ is the sensitivity map for the $$$z^{th}$$$ slice, $$$y_{MB}$$$ is the MB data, $$${\lambda _L}$$$ is the weight for the low-rank constraint, $$${\lambda _S}$$$ is the weight for the temporal frequency sparse constraint, $$$T$$$ is the temporal sparsity operator, $$$m = \left(
{\begin{array}{*{20}{c}}
{{m_1}}\\
{{m_2}}\\
\vdots \\
{{m_{{N_s}}}}
\end{array}} \right) =
\left( {\begin{array}{*{20}{c}}
{{L_1} + {S_1}}\\
{{L_2} + {S_2}}\\
\vdots \\
{{L_{{N_s}}} + {S_{{N_s}}}}
\end{array}}
\right)$$$ represents concatenated $$$N_s$$$ coil-combined images undergoing reconstruction as $$$L+S$$$ for all slices, $$$m_z$$$ is the coil-combined image4 of the $$$z^{th}$$$ slice, $$$L = \left(
{\begin{array}{*{20}{c}}
{{L_1}}\\
{{L_2}}\\
\vdots \\
{{L_{{N_s}}}}
\end{array}}
\right)$$$, $$$S = \left(
{\begin{array}{*{20}{c}}
{{S_1}}\\
{{S_2}}\\
\vdots \\
{{S_{{N_s}}}}
\end{array}}
\right)$$$, $$$P = \left( {{P_1},{P_2},...,{P_{{N_s}}}} \right)$$$, $$$Q = \left(
{\begin{array}{*{20}{c}}
F& \cdots &0\\
\vdots & \ddots & \vdots \\
0& \cdots &F
\end{array}}
\right)$$$ and $$$E = \left(
{\begin{array}{*{20}{c}}
{{E_1}}& \cdots &0\\
\vdots & \ddots & \vdots \\
0& \cdots
&{{E_{{N_s}}}}
\end{array}}
\right)$$$.
We use variable splitting5 to decompose
the problem into two subproblems: 1) the MB data consistency subproblem written as $$$\mathop {\arg \min }\limits_{{m_1},{m_2},...{m_{{N_s}}}} {\left\| {Hm - {y_{MB}}} \right\|^2} + {\mu ^2}{\left\| {m - \widehat m} \right\|^2}$$$, and 2) the slice-L+S subproblem written as $$$\mathop {\arg \min }\limits_{{{\widehat
m}_1},{{\widehat m}_2},...{{\widehat m}_{{N_s}}}} {\lambda _L}{\left\| L
\right\|_*} + {\lambda _S}{\left\| TS \right\|_1} + {\left\| {m - \widehat m}
\right\|^2}$$$. Here, $$${\mu ^2}$$$ was empirically chosen as 0.4.
We define the
conjugate of $$$H$$$
as $$${H^*} = {E^*}{Q^*}{P^*}$$$ (Figure 1D) and redefine $$${Q^*} = \left( {\begin{array}{*{20}{c}} {{F^{ - 1}}{K_1}}& \cdots &0\\ \vdots & \ddots & \vdots \\ 0& \cdots &{{F^{ - 1}}{K_{{N_s}}}} \end{array}} \right)$$$, where $$$K_z$$$ is a
matrix that performs a convolution using the split slice-GRAPPA kernel (SP-SG)6.
For comparison, a k-t
slice-SPARSE-SENSE method (Figure 1A) using the temporal total variation7 (TV) as a constraint is formulated in Equation 2:
$$\mathop {\arg \min
}\limits_{{m_1},{m_2},...{m_{{N_s}}}} {\left\| {H\left(
{\begin{array}{*{20}{c}}
{{m_1}}\\
{{m_2}}\\ \vdots \\
{{m_{{N_s}}}}
\end{array}} \right) -
{y_{MB}}} \right\|^2} + {\lambda _1}{\left\| {T\left( {\begin{array}{*{20}{c}}
{{m_1}}\\
{{m_2}}\\ \vdots \\
{{m_{{N_s}}}}
\end{array}}
\right)} \right\|_1} , (2)$$
where $$${\lambda _1}$$$ is empirically chosen as 0.01.
Methods
A saturation-recovery gradient-echo sequence was
modified to use MB excitation with CAIPIRINHA8 phase
modulation and Poisson-disk k-t undersampling. Imaging was performed on a 1.5T system (Aera,
Siemens) using 20-34 receiver channels. Single-band calibration data were
acquired in the first heartbeat, and were used to calibrate SP-SG kernels and in-plane sensitivity maps. Six-fold aggregate acceleration
was achieved using MB=3 and rate-2 (R=2) k-t undersampling. We implemented
slice-SPARSE-SENSE and slice-L+S methods in MATLAB, both based on SP-SG and MB CG-SENSE9, where slice-SPARSE-SENSE used
temporal TV compressed sensing6, and slice-L+S used
low-rank and temporal-frequency sparsity and were solved using CG10,11
and soft thresholding with variable splitting4. The methods were evaluated in six patients, with 9 slices per patient. The two reconstruction methods
were scored (1-5, 5 is best) by two cardiologists. Results
2DIFFT-reconstructions illustrate the artifacts
associated with MB=3 and R=2 sampling (Figure 2a), and initial SP-SG reconstructions with remaining R=2 undersampling and
slice-separation artifacts are shown in Figure 2b. Example images demonstrating the slice-L+S method are shown in Figure 2c, showing simultaneous decomposition
of background and dynamic components for multiple slices. Subsequently, the superposition
of L and S demonstrates slice separation and artifact removal (Figure 2d). The example (Figure 3A) compares slice-SPARSE-SENSE and
slice-L+S, where slice-L+S shows sharper borders and greater contrast. The cardiologist
scoring results were 3.8 ± 0.58 and 4.1 ± 0.36 for slice-SPARSE-SENSE
and slice-L+S, respectively (Figure 3B). Figure 4 shows a slice-L+S example of nine-slice coverage.Discussion
We developed slice-SPARSE-SENSE
and slice-L+S reconstructions that use through-plane and in-plane coil
information, consistency with the acquired data and that enforce temporal constraints. CAPIRINHA phase modulation (MB=3), Poisson-disk (R=2)
undersampling and proposed reconstructions provide an effective means to
acquire and reconstruct MB first-pass perfusion images. Slice-L+S provides sharper
borders and greater contrast than slice-SPARSE-SENSE with temporal TV, though
more studies need to be performed. These methods enable the acquisition
of nine slices in the time typically required to acquire three slices. Acknowledgements
This work was supported by R01HL147104 and R01HL131919.References
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