Hongfu Sun1, M. Ethan MacDonald1, and G. Bruce Pike1
1University of Calgary, Calgary, AB, Canada
Synopsis
A method to remove phase offsets in bipolar gradient-echo readouts is proposed. Their effects on Quantitative Susceptibility Mapping (QSM) reconstruction are demonstrated by comparing QSM before and after phase offsets removal. Purpose
To demonstrate a method that removes phase
offsets from a multi-echo bipolar gradient-echo acquisition, and investigate
the effect of the phase offset correction on quantitative susceptibility map
(QSM) reconstruction.
Methods
In a gradient-echo sequence, phase
accumulates linearly with echo time in addition to an initial phase offset:
$$$\phi=-\gamma\cdot\Delta{B}\cdot{TE}+\phi_{0}$$$, where $$$\phi$$$ is the measured
phase at $$$TE$$$ and $$$\phi_{0}$$$ is the initial phase offset. However, in multi-echo
bipolar gradient-echo readouts, the phase offsets in odd and even echoes are
different, and simple linear regression with non-zero intercept introduces
errors for QSM [1,2]. Here we propose a method to remove phase offsets in both
odd and even echo readouts completely, and then perform a linear regression
with zero intercept.
Consider all the odd echo readouts first: a
phase difference map between the first two odd echoes was generated through the
division of the raw complex images ($$$S$$$): $$\Delta\phi=\angle(S_2\cdot
S_1^*)=-\gamma\cdot\Delta B\cdot\Delta TE.$$ After unwrapping the phase
difference map $$$\Delta\phi$$$ and obtaining $$$\Delta\Phi$$$, using a
path-based method such as PRELUDE of FSL package, the phase evolution at
$$${TE}_1$$$ without offset can be estimated as:
$$\Phi_1=\Delta\Phi/\Delta{TE}\cdot {TE}_1.$$ The phase offset can then be
calculated by complex division of estimated phase at $$${TE}_1$$$ from the measured complex image at $$${TE}_1$$$: $$\phi_0=\angle (S_1 \cdot \exp(j \Phi_1)^*).$$
Finally, offset corrected phase can be computed by removing estimated offset from the complex image: $$\phi_{corr}=\angle (S
\cdot \exp(j \phi_0)^*).$$ Phase offset in the even echoes was removed
following the same process.
After phase offsets correction, QSM can be reconstructed following the
pipeline of (1) spatial phase unwrapping of each echo using PRELUDE, (2) magnitude-weighted
least-square fitting of the unwrapped phase with zero intercept, (3) background field removal using
RESHARP, and (4) dipole inversion using total variation regularization.
Ten healthy subjects were scanned using a three-dimensional bipolar
gradient-echo acquisition at 3 T (GE Healthcare). The parameters were: 25.6 x
25.6 x 12.8 cm$$$^3$$$ FOV, 1 mm isotropic spatial resolution, 8 bipolar echoes
with a first TE of 2 ms and a 2.4 ms echo spacing thereafter, 22 ms TR, 488
Hz/pixel bandwidth, ASSET = 2 parallel imaging, and a total scan time of 3 mins
50 secs. QSM reconstructions with and without the correction procedure outlined
above were performed.
Results
The effect and removal of phase offsets in
odd and even echo readouts is demonstrated in Fig. 1. In the top two rows, odd
and even echo readouts display asymmetric phase wrap patterns. After removing
the odd and even echo offsets from the respective echoes, the corrected phase
images display symmetric wraps that evolve with echo times, as shown at the
bottom rows. Average phase values in the blue circle region-of-interest in Fig.
1 were measured across the 8 echoes and are plotted in Fig. 2, both before and
after offset correction. The raw phase from the bipolar readout shows large jumps
between odd and even echoes, as opposed to the linear phase evolution after
correction. The residuals of fitting the unwrapped phase with echo time are
also shown in Fig. 2. The
voxel-based fitting residuals are substantially reduced after phase offset
correction. QSM images derived from phase uncorrected and corrected data are
superficially similar, however, if examined carefully it is clear that the
phase corrected QSM images have improved image quality and significantly
reduced artifacts around vessels (Fig. 2 right column).
Discussion
Bipolar gradient phase correction has been
proposed in a previous paper [2], using the first three echoes to remove the
offset difference between odd and even echoes. Here we propose to directly remove
the odd and even echo offsets from all the respective echoes. We then linearly
fit the unwrapped phase with a zero intercept. We implement our method in a complex
manner that reduces the need for a phase unwrapping process for the offset correction.
For example, in the previous method, phase maps from each of the first three
echoes need to be unwrapped, while in our method only the phase difference is
unwrapped once. QSM failures have been reported if reconstructed without
bipolar phase offset correction [2]. Interestingly, we did not observe any
failed QSM’s reconstructed without offsets correction, though the QSM image
quality was degraded. This may be due to the symmetry of the phase offsets
between the uncorrected odd and even echoes, as observed in Fig. 2, and the
robustness of our QSM pipeline. However, with the phase offsets correction
proposed here, we observed a significant reduction in artifacts around some
vessels in all the ten subjects.
Acknowledgements
Funding supports from Campus Alberta Innovates Program (CAIP) and Canadian Institutes for Health Research (CIHR).References
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Catalytic multiecho phase unwrapping scheme (CAMPUS) in multiecho gradient echo
imaging: removing phase wraps on a voxel-by-voxel basis. Magn Reson Med. 2013
Jul;70(1):117-26.
[2] Li J, Chang S, Liu T, Jiang H, Dong F,
Pei M, Wang Q, Wang Y. Phase-corrected bipolar gradients in multi-echo
gradient-echo sequences for quantitative susceptibility mapping. MAGMA. 2015
Aug;28(4):347-55.