Ying Chen1, Song Chen1, Hui Liu2, and Jianhui Zhong1,3
1Center for Brain Imaging Science and Technology, Zhejiang University, Hangzhou, China, People's Republic of, 2MR Collaboration Northeast Asia, Siemens Healthcare, Shanghai, China, People's Republic of, 3Collaborative Innovation Center for Diagnosis and Treatment of Infectious Diseases, Zhejiang University, Hangzhou, China, People's Republic of
Synopsis
Single-shot GE-EPI is widely used in
fMRI. However, it is susceptible to field inhomogeneity induced geometric
distortions, therefore retrospectively unwarping of the single-shot GE-EPI data
is important. A commonly used unwarping technique is based on the field map
of the image and it would be desirable to acquire the field map at each
time point of a dynamic fMRI measurement series. The aim of this abstract
is to qualitatively and quantitatively compare the performance of three reference-free
unwarping methods on human brain imaging data. Experimental results demonstrate that the field map obtained from measuring the k-space shifts of each voxel can provide more reliable unwarped images.Purpose
Single-shot GE-EPI is widely used in fMRI. However,
it is susceptible to field inhomogeneity induced geometric distortions,
therefore retrospectively unwarping of the single-shot GE-EPI data is important
for accurately co-registering functional images with structural images.
A commonly used unwarping technique is based on field map of image,
which is often acquired at the beginning of experiments. However its reliability may be compromised by motions and physiological activities of subjects during experiments, and thus the field map is desired at each time point of a dynamic fMRI
measurement series. The field map in distorted coordinates can be
obtained from the phase data by a proper phase unwrapping procedure
1. Alternatively, it can also be calculated by integrating the off-resonance
gradient maps which can be obtained from analyzing the k-space echo shifting of
each voxel
2-3, or from calculating the phase differences of two
adjacent voxels
3. The aim of this work is to qualitatively and
quantitatively compare the performance of the above-mentioned three reference-free unwarping methods on
human brain data.
Methods
The data processing schemes of the three unwarping
methods are shown in Fig.1.
Human brain data
of one healthy volunteer were acquired on a Siemens 3T Prisma scanner with
informed consent, using a 20-channel head coil and the built-in BOLD sequence. Three orthogonal orientations were scanned with fat
suppression, 24 slices for each. FOV=220×220mm2 with slice thickness=5mm, TR/TE=3000ms/30ms,
acquisition matrix=64×64, SW=2440Hz/voxel, echo spacing=490μs. Referential TSE images were scanned with
TR/TE=5000ms/104ms and acquisition matrix=256×256.
Results and discussion
The unwarping
results of representative slices are shown in Fig.2. Two slices are selected for
each orientation, one with relatively large deviation in the estimated
off-resonance frequency values (Δf) obtained
from the three field map calculation procedures, and the other with
minor difference. Visual inspection suggests that most of the
distortions can be corrected by all three methods, and generally k-space filtering method produced relatively more stable
unwarping results than the other two methods.
Furthermore,
quantitative investigation were conducted.
First, the SNR
of selected areas were calculated. Figure 3 shows that unwarping
procedures led to the reduction of SNR and apart from some specific slices,
the SNR obtained from three unwarping methods were very close.
Secondly, the
disparity of the field maps obtained from three methods were
evaluated by calculating the root-mean-squares deviation of the estimated
Δf between each two methods in the labeled areas of the previous study, and the results are shown in Fig.4. For traversal orientation, since vertical
stretching existed for most of the slices and k-space filtering method generally
achieved better unwarping performance, Δf obtained by it
presented larger deviation from the values obtained by the other
two methods. For coronal and sagittal orientations, since distortions
were regional, three methods achieved similar unwarping quality for most of
the slices except for some small differences at regional profiles. The
estimated Δf were also very close, especially for what
was obtained by k-space filtering and phase difference methods because they
shared similar gradient map integration strategy.
Thirdly, the
variation tendency of the estimated off-resonance frequency values from the
data acquired by different coils was measured. Based on Fig. 4, for each
orientation one slice with relatively small deviation between 3 field maps was
selected to study. Two areas were measured on them, one was relatively
homogeneous and immune to distortions, the other with relatively large field
gradients and susceptible to distortions. Figure 5 shows that the homogeneous
regions resulted in smaller variations of Δf
compared with the inhomogeneous regions. The k-space filtering and phase
unwrapping methods gave rise to larger variations than phase difference method because
both the determination of accurate k-space shifts and phase values depend more
closely on the SNR of acquired data.
Conclusion
Both qualitative
and quantitative experimental results demonstrate that k-space filtering
method can provide more stable unwarping performance and SNR level than the
other two methods attributed to two reasons. First, the off-resonance
gradient map obtained is of higher SNR than phase difference
method; secondly, the underlying local linear fitting involved can help provide
more accurate field map than phase unwrapping method, especially at regions
with large field gradients.
Because the
estimated off-resonance frequency values vary with coil, combining the field
maps obtained from different coils with corresponding sensitivity distribution improved the accuracy of the
estimated field map by making it less dependent to the selection of initial seed in related
region-growing process
4, which would facilitate the automatic
processing of large amounts of data in fMRI.
Acknowledgements
No acknowledgement found.References
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