Young Joong Yang1,2, Jong-Hyun Yoon1, Jinho Park1, Hyeon-Man Baek2, and Chang-Beom Ahn1
1Kwangwoon University, Seoul, Korea, Republic of, 2Korea Basic Science Institute, Ochang, Korea, Republic of
Synopsis
A tissue characterization with
susceptibility e.g., susceptibility weighted imaging (SWI), quantitative
susceptibility mapping (QSM), susceptibility tensor imaging (STI), gets more
attention in high field MRI. Using a numerical phantom, various processing
elements for QSM are analyzed. We propose a method to remove background phase
using a discrete wavelet transform (DWT). The proposed DWT method shows
superb performances over exiting techniques including SHARP in the QSM
experiments with volunteer subjects at 7.0T and 3.0T MRI, without distortions
at the susceptibility maps.Purpose
A tissue characterization with
susceptibility e.g., susceptibility weighted imaging (SWI), quantitative
susceptibility mapping (QSM), susceptibility tensor imaging (STI), gets more attention
in high field MRI. We propose a method
to remove background phase using a discrete wavelet transform (DWT) by which
slowly varying low frequency distortions are substantially reduced in the
resultant susceptibility map compared to existing techniques.
Methods
In general three processing steps
are needed in the QSM analysis: phase unwrapping, background phase removal, and
susceptibility mapping or reconstruction by solving an inverse problem. The former two steps are preprocessing needed
to obtain accurate susceptibility maps.
Various phase unwrapping methods have been proposed
1,2.
Background phase results from global geometry, air-tissue interfaces, and any
field inhomogeneity, which needs to be removed, thereby leaving the phase only due
to tissue susceptibility. To remove the background phase, Laplace equation (sum
of the second order partial derivatives of the background phase along x, y, and
z directions makes zero) is used. There
are several ways to implement the Laplace equation in the forms of convolution
and deconvolution at the spatial and spatial frequency domains
3. Some (wrinkle like) low frequency distortions
are observed in the reconstructed susceptibility maps similar to Gibbs
phenomena, which are partially due to the division of the Laplacian kernel in the
spatial frequency domain to implement the deconvolution process.
We propose a method to remove the background phase
by DWT. Three dimensional DWT is applied iteratively for decomposing the phase
images into high and low frequency bands.
Three stage decompositions are made by using a 4th order
symlet wavelets, a modified version of Daubechies wavelets. The background removed phase images are
obtained by reconstructing the decomposed images without the lowest frequency
band. Since the background phase
consists of local dc and linear terms mostly, they can be removed by a high
pass filtering
4. Since DWT is
performed entirely in the spatial domain, no conversion or division of the Laplacian
kernel in the spatial frequency domain is needed, which reduces the low
frequency distortions in the susceptibility map.
Results
Various background phase
removal methods are tested with a series of parameters for a numerical phantom which
consists of 12 cylinders with different susceptibilities from 0.02 to 0.24
ppm. Figure 1 shows the susceptibility
maps obtained by removing the background phase with SHARP 3, and the
proposed DWT method. Other processing
procedures including phase unwrapping and susceptibility reconstruction were
the same for both cases. The susceptibility values reconstructed in the 12
cylinders of the phantom are also shown.
As seen in Fig.1, more accurate susceptibility map is obtained by using
the DWT method compared to SHARP. Figure
2 shows in-vivo susceptibility maps of head for volunteers obtained at 7T and
3T MRI. Three dimension gradient echo
sequence was used to obtain the phase images. Two echoes were obtained with TR=30ms,
TE1=8.1ms, TE2=20.3ms, flip angle=10 degrees, FOV=224x224x40mm, matrix
size=448x448x40. The phase images were obtained by subtracting the phase of the
first echo from that of the second echo.
As seen in Fig.2, low frequency distortions are dominant in the
susceptibility map using SHARP (a), while such artifact is not seen in the map using
DWT (b) (see the ellipses marked). The distortions are more serious at higher
field (7T).
Discussion
From computer simulation using
a numerical phantom and in-vivo experiments at 7T and 3T MRI, more accurate
susceptibility maps are obtained when the background phase is removed by DWT
compared to other existing techniques including SHARP. Since DWT applies entirely in the spatial
domain, no conversion or division of the kernel in the spatial frequency domain
is needed, which reduces low frequency distortion in the resultant
susceptibility maps. More theoretical
background of the DWT on relationship with the Laplace equation may need to be further
investigated.
Conclusion
Using a numerical phantom,
various processing elements for QSM are analyzed. The computer simulation shows that the DWT
method efficiently removes the background phase without introducing low
frequency distortions at the resultant susceptibility maps. The proposed DWT method also shows superb
performances over exiting techniques in the QSM experiments with volunteer
subjects at 7.0T and 3.0T MRI, without slowly varying distortions at the
susceptibility maps.
Acknowledgements
This work was supported by the National Research Foundation of Korea(NRF) grant funded by the Korea government(MSIP) (NRF-2015R1A2A2A03005089).References
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