Fuyixue Wang1, Zijing Dong1, Shuo Chen2, Bingyao Chen3, Jiafei Yang3, Xing Wei3, Shi Wang2, and Kui Ying2
1Department of Biomedical Engineering, Tsinghua University, Beijing, China, People's Republic of, 2Key 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, 3Department of Orthopedics, First Affiliated Hospital of PLA General Hospital, Beijing, China, People's Republic of
Synopsis
Real time thermometry is desirable for thermal
therapy such as microwave ablation to ensure patient safety. MR temperature imaging
using proton resonance frequency (PRF) shift technique can provide temperature
maps during the treatment. In this work, we proposed a novel reconstruction
framework that estimates temperature changes from undersampled k-space with a
few fully sampled k-space points. Simulation studies, phantom heating
experiments and human experiments were performed to validate the proposed
method. The proposed method can provide temperature images with relatively high
accuracy and short reconstruction time at a reduction factor of 4 in presence
of motion.Target Audience
Radiologists and scientists working on MR
thermometry.
Purpose
Microwave ablation is a minimally invasive
thermal therapy to kill tumor cells in various human regions. MR temperature
imaging using proton resonance frequency (PRF) shift technique 1 allows us to
monitor temperature during the treatment. To ensure patient safety, acceleration
of data acquisition is required to obtain temperature images with high temporal
resolution. Besides, techniques reducing motion artifacts are also needed
especially in abdominal organs. K-space method 2 based on hybrid model 3 is
an effective solution to these issues, but this approach becomes inaccurate when motion states
are not covered by the baseline library and its reconstruction time is relatively long
for real time temperature mapping.
In this study, we developed an accelerated
temperature estimation method with relatively short reconstruction time and high
temperature accuracy in presence of the motion not covered by baseline library.
Methods
Theory: The
proposed method estimates temperature changes from undersampled k-space based
on the hybrid model 3. Different from the conventional k-space method 2, several
lines in the center of k-space are acquired in addition to the uniform undersampling
acquisition to get low resolution images. These low resolution images are used
to match the baseline images and eliminate phase shifts due to magnetic field
drift. In this way, we can avoid the loop iterations of the conventional
k-space method in order to speed up the estimation, and reduce the steps to
adjust the sparsity coefficient during the process of reconstruction. Rigid registration
is also implemented to further correct temperature errors due to the
displacement of the subject by utilizing the center k-space data. The main
steps of the proposed method are shown in Fig. 1.
Experiments: A phantom simulation was performed to simulate a
Gaussian-shaped heat-induced phase shift (maximum temperature change: 30℃, standard deviation: 2.5 pixels) on
the heating target.
To evaluate the ability of the proposed method to estimate
temperature when the motion states are not covered by the baseline library, motion
simulation was performed to simulate a moving process of the object. The
simulated baseline images consisted of 11 images in which the object was moved
2 pixels/frame along the frequency encoding direction from -10 pixels to 10
pixels relative to the starting point. The moving process during the treatment
was then simulated in which the object was moved at a speed of 2 pixels/frame
from 10 pixels to -10 pixels in the first 12 frames and moved 1 pixel/frame
back to 10 pixels in the last 20 frames as shown in Fig. 3c. So the first
twelve positions were all included in the baseline library, while half of the
last twenty positions were not.
To verify
the ability of the proposed method to estimate temperature changes in practice,
a phantom heating experiment was performed using an MR-compatible microwave
probe (Nanjing ECO Microwave System Co., Ltd, Nanjing, China). A fiber optic
thermometer was inserted into the phantom next to the microwave heating probe.
In-vivo
non-heated experiment was also performed to acquire spinal cord images on
healthy volunteers with free-breathing. The standard deviations of different
time points were calculated for comparison.
Fully
sampled k-space data were acquired with the 2D FFE sequence on a 3.0T Phillips scanner
(Philips, Best, the Netherlands) and then retrospectively under-sampled. Reconstructed
temperature maps of the proposed method were compared with SPIRiT 4 and the
conventional k-space estimation reconstruction thermometry 2 using the same
undersampling pattern.
Results
The results of phantom heating simulation are
shown in Fig. 2. The proposed method results in the lowest RMSEs and uses much
shorter time than the conventional k-space method. Fig. 3 shows the results of
motion simulation. There are smaller motion-induced temperature errors using
the proposed method. The results of phantom heating and in-vivo experiment are
shown in Fig. 4 and Fig. 5. The temperature evolution curve of the proposed
method agrees well with the optical fiber (Fig. 4a) and the spatial standard
deviations of the proposed method are much less than the conventional k-space
method in in-vivo data (Fig. 5).
Discussion
Both the phantom heating simulation and the phantom heating experiment
demonstrate the ability of the proposed method to estimate temperature with
less computation time and higher accuracy. Motion simulation and in-vivo
experiment further show the feasibility of the proposed method for monitoring
temperature in presence of motion.
Conclusion
The proposed method can accelerate MR
thermometry at an acceleration factor of 4 and provide temperature maps with improved accuracy and robustness to motion, which makes real time imaging for
MR-guided microwave ablation possible.
Acknowledgements
This work is supported by National Nature Science Foundation of China, 61571257. The authors acknowledge and thank William Grissom for suggestions. References
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