Fuyixue Wang1, Zijing Dong1, Haikun Qi2, Shi Wang3, Huijun Chen2, and Kui Ying3
1Department of Biomedical Engineering, Tsinghua University, Beijing, China, People's Republic of, 2Center for Biomedical Imaging Research, Department of Biomedical Engineering, School of Medicine, Tsinghua University, Beijing, China, People's Republic of, 3Key Laboratory of Particle and Radiation Imaging, Ministry of Education, Medical Engineering and Institute, Department of Engineering Physics, Tsinghua University, Beijing, China, People's Republic of
Synopsis
Real
time MR temperature imaging during thermal therapy is beneficial for monitoring
and controlling the treatment in clinical applications. In this work, we
explored correlations in the temporal dimension of temperature imaging and
proposed a novel method, temporal weighted sliding window SPIRiT using
motion-insensitive golden angle radial sampling, to achieve real time
temperature imaging. Through simulation studies and phantom heating
experiments, we validated the ability of the proposed method to obtain temperature
images with relatively high temperature accuracy at a reduction factor of 8.Target Audience
Radiologists and scientists working on MR
thermometry.
Purpose
Real
time MR temperature imaging during
thermal therapy is beneficial for monitoring and controlling the treatment. Therefore,
high spatiotemporal resolution is required for clinical applications. In recent
years, several reconstruction methods have been proposed to explore correlations
in temporal dimension for a high acceleration factor, such as reconstruction
methods based on k-t space (k-t GRAPPA 1, k-t SPIRiT 2). However, these
methods are not easy to achieve real-time temperature monitoring because the
information from the future time points is needed to get unbiased
temperature estimation.
In this work, we proposed a novel method, temporal weighted
sliding window SPIRiT using motion-insensitive golden angle radial sampling to
achieve real time temperature imaging.
Methods
Theory: In the proposed method, the k-space data from
several previous time frames are used to reconstruct the target temperature map
by solving the following optimization problem based on SPIRiT 3:$$argmin(
d_{c} ) \quad \parallel W_id_r-Dd_c
\parallel^{2}_2+\lambda\parallel(G-I)d_{c}\parallel^2_2$$
where $$$d_c$$$ is the reconstructed
Cartesian k-space data of all channels at current time frame, $$$d_r$$$ is the acquired radial k-space data, $$$W_i$$$ is the temporal weight of $$$d_r$$$ at the $$$i$$$th iteration, $$$D$$$
represents a gridding matrix for non-Cartesian sampling which also selects the
acquired k-space points out of $$$d_c$$$, $$$G$$$ is the SPIRiT interpolation
operator, $$$I$$$ is the identity matrix, $$$λ$$$ is the regularization parameter to adjust
data consistency and calibration consistency.
A
weighted sliding window covering the present k-space data and several k-space
data form previous time frames is used to create a k-space with relatively more
acquired points for data consistency and calibration process. In this way,
there is no need to take extra k-space data for calibration, which are done by the
conventional SPIRiT and k-t SPIRiT. And to avoid temperature estimation bias
from data of previous time frames, the weight of k-space data from previous
time frames is iteratively reduced while repeatedly solving the above
optimization problem.
Experiments: A
phantom simulation was performed to simulate heat-induced phase shifts with
maximum temperature change of 30℃
on a 1% agar phantom.
A phantom experiment was also performed to evaluate the
proposed method. A cooling down process was scanned after the agar phantom was
heated to about 50℃ at
the beginning of the experiment.
All images were obtained on a 3.0T Phillips
scanner (Philips, Best, the Netherlands) with a
time-interleaved Golden Angle sampling scheme with following parameters: FOV=16cm, matrix size=80×80, 100
projections, 160 readout points, TR/TE=50/10ms. The correction of
gradient errors from radial sampling was performed on all data using TrACR 4 and fully sampled data were undersampled with a reduction factor of 8×(12
projections) for reconstruction. The proposed method was compared with
frame-by-frame SPIRiT 3 and non-weighted temporal SPIRiT.
Results
Fig.
1 shows the estimated temperature maps and temperature errors using the three
methods in simulation. Compared with frame-by-frame SPIRiT and non-weighted
temporal SPIRiT, the proposed method results in lower temperature errors in
heated region and its surrounding area. The temperature evolution curve of the
proposed method agrees well with the fully sampled data (Fig. 2). The results
of the phantom cooling down experiment are shown in Fig. 3 and Fig. 4. The
proposed method provides closest temperature estimation to the fully sampled
data with RMSE of about 0.2℃.
Table1 illustrates the RMSEs of
ROI (7×7 voxels in heated region) at three different time frames in the simulation
and the phantom cooling down experiment. The RMSE of ROI at the 15th time frame
using non-weighted temporal SPIRiT in the simulation reached to 5.16℃ because of temporal delay response. In
comparison, the proposed method results in lower RMSEs at the three time frames
chosen.
Discussion and
Conclusion
Compared with other approaches,
the proposed method improves the accuracy of temperautre estimation, not only
by utilizing the information from previous time frames, but also by emphasizing
the information of the current time frame via decreasing temporal weights of
previous time points. The weighted sliding window uses only the previous data
rather than the data collected during the whole monitoring process.
This
prospective implementation helps the real-time temperature monitoring to be feasible.
In-vivo experiments are under way to further test the feasibility of the
proposed method on human data in the presence of respiratory motion.
Acknowledgements
This work is supported by National Nature Science Foundation of China, 61571257.References
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