Synopsis
Chemical shift encoding-based water-fat imaging, or Dixon imaging, is of
recent interest in MRA. Single-echo Dixon methods are particularly appealing for
this application because of their potential for decreasing scan times. This
work suggests modifications to existing single-echo Dixon methods and
demonstrates their benefits, primarily improvements in SNR and CNR, in contrast-enhanced
peripheral MRA.Introduction
Single-point Dixon methods attempt to separate water and fat signal from a
single image only. They are fundamentally limited in their ability to resolve mixed
water and fat signal without additional a priori information, for instance on
the present main field inhomogeneity. Nevertheless, single-point Dixon methods seem attractive, since they promise a substantial reduction in scan time compared
to multi-point Dixon methods. This holds in particular for applications that
are on the one hand time-critical and on the other hand undemanding as to the
accuracy of the separation. Among these is notably contrast-enhanced MRA, in
which a reasonable fat suppression is often sufficient. The purpose of this
work was to improve single-point Dixon imaging in terms of SNR and CNR primarily in this application.
Theory
The measured signal
S is modeled in image space as
$$S=(W+cF)p,$$
where
W
and
F denote the water and fat
signal,
c a factor describing the evolution
of a pure fat signal in the absence of main field inhomogeneity, and
p a phase error.
p is derived either from
S, assuming that either water or fat is present in individual voxels, or from other sources, such as an additional
reference scan
1,2.
W and
F are then obtained by
$$F=Im\{S/p\}/Im\{c\},$$
$$W=Re\{S/p\}-F\cdot Re\{c\}.$$
Setting $$$c=e^{2\pi f_F \text{TE}}$$$, where
fF denotes the resonance frequency offset of fat relative
to water and TE the echo
time, the SNR in the water image is reduced by a factor of $$$sin(2\pi f_F \text{TE})$$$ relative to the
SNR in the measured image.
To avoid loss of water signal, in particular
for $$$Re\{c\}<0$$$, it is proposed to impose non-negativity constraints
on
W and
F, for instance by
$$F=max\{Im\{S/p\}/Im\{c\},0\},$$
$$W=max\{Re\{S/p\}-F\cdot Re\{c\},0\}.$$
Moreover, to limit loss of SNR, especially
for less favorable TEs, it is suggested to replace
W or
F by
S if the estimated
W
and
F indicate a strong dominance of
one of the signal, for example by
$$F'=abs\{S\}, W'=0,$$
if $$$F>t W$$$, and
$$F'=0, W'=abs\{S\},$$
if $$$W>t F$$$, with a suitable threshold $$$t \geq 1$$$.
Methods
The described modifications
were evaluated in subtractionless first-pass peripheral MRA
3. Data were acquired
on patients on a 1.5 T Ingenia scanner (Philips Healthcare, Best, Netherlands).
After injection of 0.1 mmol/kg Gadobutrol (Bayer Healthcare, Berlin,
Germany), contrast-enhanced images were collected with a 3D T
1-weighted
spoiled dual-gradient-echo sequence (TE
1/TE
2 = 1.8
ms/3.0-3.2 ms) at three stations. For the purpose of this work, only the images from
the first gradient echo were used.
Results
A
selected slice of one of the contrast-enhanced images is shown in Fig. 1.
p was derived from the image itself in
this case. The division by
p removed
the phase variations induced by main field inhomogeneity reasonably well,
except in the heels. The application of the original single-point Dixon method to the corrected
image yielded the water and fat images in Fig. 2. Due to the TE of 1.8 ms, at
which the dephasing of water and fat signal amounts to about 2.5 rad or 140°, the
SNR is noticeably reduced, especially in the water image. Corresponding water and fat images
obtained with the modified single-point Dixon method are provided in Fig. 3.
The SNR is evidently improved, as is the vessel-to-background contrast or CNR.
The latter is particularly striking in the MIP and the difference images in Fig. 4.
Discussion
Due
to the presence of contrast agent and of flow, the phase in the vasculature may
differ from the phase in surrounding non-fatty tissue. This may lead to negative
fat signal and reduced water signal in the vasculature using the original
single-point Dixon method, whereas the proposed non-negativity constraints effectively
prevent this. The choice of the TE in single-echo Dixon imaging is typically
more critical to attain an adequate SNR than the choice of the TEs in
multi-echo Dixon imaging, which compromises the expected reduction in scan
time. The suggested selective, direct propagation of the measured signal to the
water or fat signal may avoid the SNR penalty associated with less favorable TEs
to a large extent and thus provide more flexibility in optimizing the employed sequence.
Acknowledgements
No acknowledgement found.References
1. Yu H, et al. Magn Reson Med 2006; 55:413-422. 2.
Ma J. J Magn Reson Imaging 2008; 27:881-890. 3. Leiner T, et al. Eur Radiol 2013; 23:2228-2235.