Cheng Junying1, Xu Man1, Mei Yingjie2, Liu Liang1, Feng Yanqiu3, and Cheng Jingliang1
1Magnetic Resonance Department, The First Affiliated Hospital of Zhengzhou University, Zhengzhou, China, 2Philips Healthcare, Guangzhou, China, 3School of Biomedical Engineering, Southern Medical University, Guangzhou, China
Synopsis
The
accurate recovery of underlying true phase is
vital for a large number of applications, such as water/fat separation, quantitative susceptibility mapping and brain imaging. In this work, we propose a 3D phase unwrapping method based on phase partition and local polynomial fitting. The simulated
and in vivo experiments demonstrate the proposed method can obtain perfect
unwrapped results even in the regions with low SNR and rapidly changed phase,
and can be applied to the abdominal QSM.
Target Audience
Researchers
who are interested in phase unwrapping (PU) and abdominal quantitative
susceptibility mapping.Purpose
In
MRI, the acquired signal is combined by magnitude and
phase. The magnitude is usually used while phase discarded in clinical
diagnosis. The acquired phase is generally wrapped back into (-π, π] range. However,
accurate recovery of underlying true
phase is vital for a large number of applications, such as water/fat
separation [1], quantitative susceptibility mapping [2] and brain imaging [3].
A large
number of PU algorithms have been proposed, while most of them are generally
challenged by noise and rapid phase change. In this work,
we propose a 3D PU method based on the phase partition [4] and local polynomial fitting.
The proposed method first clusters the input phase map into blocks by phase partition method. The blocks with
the voxels less than a predefined threshold are classified into residual voxels.
After that, the proposed method sequentially performs inter-block and residual voxel
PU by the local polynomial fitting. The unwrapping starts with the
largest block, and proceeds with the nearest blocks and voxels. The 3D simulation
and in vivo abdominal data were implemented to evaluate the performance of the
proposed method with comparisons to the PRELUDE [4], graph-cut [5], region-growing [6]
and Laplacian_based methods [7].Methods
In the VOI, the phase interval (-π, π] is partitioned into equispaced
subintervals. For each subinterval, a mask
of voxels whose phase values are within this subinterval is generated. Then, blocks
are identified by detecting connected components. The blocks with
voxels less than a threshold are classified into residual voxels. A unique index is assigned to each block. The phase of every voxel in one
block has a common integer offset; thus, each block can be treated as a unit.
The largest block is selected as the starting block. The growing-block is
selected by considering the Euclidean distance between between each block. The local polynomial fitting approach is
implemented on the voxels in the growing-block that are closest to the
unwrapped regions and the voxels in the unwrapped regions that are closest to
the growing-block to obtain the optimal integer offset for the growing-block. After all
the blocks are unwrapped, the residual voxels are
unwrapped based on the quality-guided region-growing local polynomial fitting method. The phase
derivative is calculated as the quality criterion to improve the residual-voxel
unwrapping.
To evaluate the performance
of proposed method on the simulation, two different 3D phase models were used: One is Gaussian phase ball (100×100×100): $$\mu_{x,y,z}=100\ast \mathrm{e}^{\frac{-x^{2}-y^{2}-z^{2}}{2}}$$standard deviations (SD) is 20 voxels. The magnitude increased from 10 to 100 with an increasement of 10 to consider
the affection of signal-to-noise ratio (SNR). Another is (101×101×51): $$\mu_{x,y,z}=5\ast [(\frac{sin(x)}{x})(1.50-z)+\frac{sin(y)}{y}(0.49+z)]$$which is a more generalized and complicated simulation [8].
The magnitude was set to 50. Gaussian noise with SD of 20 and 10 rad were separately
added to the two complex data. The misclassification ratio (MCR) [4] was
calculated as the incorrect unwrapped voxel ratio to quantitatively evaluate the
performance of proposed method. The simulation was repeated 30 times, and
the means and SDs of MCRs (%) were calculated.
The in vivo abdominal data [9] was obtained on a 3T MRI
scanner (Magnetom Prisma; Siemens) in 1 man volunteer using 2D gradient echo
breath-hold sequence (voxel size =1.95×1.95×5 mm3, number of slices=10, flip angle=20°, TE=4.92 ms, TR=71 ms, bandwidth=930 Hz/pixel, scan
time=7.5 seconds). The variable-radius sophisticated harmonic artifact
reduction for phase data [10] and a 2‐level QSM reconstruction algorithm called STAR‐QSM [11] with default parameters were used to remove the background
field and calculate the susceptibility map. The program was implemented
in MatLab (R2016B; MathWorks, Natick, MA) on a desktop computer.Results and Conclusion
The results of PRELUDE,
graph-cut and Laplacian-based methods contain residues (white arrows), while proposed method obtains smooth phase in Fig.1; The MCRs of
PRELUDE, graph-cut and Laplacian-based methods are separately 4.28±0.06, 2.26±0.02 and 20.65±0.02, while the proposed method MCR is 0.01±0.01.
In Figure 2, the region-growing method obtained the
worst result,
PRELUDE and graph-cut methods were suboptimum, while proposed method
acquired the perfect unwrapped map. The
MCRs of PRELUDE, graph-cut, region-growing
and proposed methods are separately
10.33±9.80, 20.71±1.19, 84.47±6.62 and 0.01±0.01.
Figure 3 shows the phase-unwrapping and QSM results of PRELUDE, graph-cut, region-growing, Laplacian-based and proposed algorithms, respectively. The open-end cutlines [1] at
the edge of the phase map (white
arrows) lead the results of the five
methods still contains discontinuities, while proposed algorithm shows the unwrapped
phase with the least residues. The resulting susceptibility maps exhibit
errors attributed to the residues for the five methods (white arrows). The five
algorithms show streaking artifacts close to the ribs (black arrows), which may
be caused by the significantly lower susceptibility of the ribs [9]. Overall, proposed algorithm displays the susceptibility map with the least
artifacts.
In this
work, a novel 3D PU method is presented.
The simulated experiments demonstrate proposed method can obtain perfect
unwrapped results even in the regions with low SNR and rapidly-changed phase. The
abdominal QSM is challenging for large changes in susceptibility and
regions with low SNR, proposed method have acquired the best results, and might
be a good option for abdominal QSM.Acknowledgements
No acknowledgement found.References
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