Nicholas R. Zwart1, Dinghui Wang1, and James G. Pipe1
1Imaging Research, Barrow Neurological Institute, Phoenix, AZ, United States
Synopsis
Time of Flight MRA in the head and neck can benefit from Dixon fat signal removal. The spiral trajectory is used to speed up the acquisition allowing 3-echoes to be collected, for Dixon reconstruction, in less time than a conventional single echo ("out-of-phase") cartesian MRA.Introduction
Magnetic resonance angiography (MRA) methods such as Time of Flight
(ToF) can benefit from fat suppression techniques in areas where the fat
signal obscures the contrast between areas of flow and static tissue [1]. The
three-point Dixon water-fat separation methods have been shown to provide
a means of removing fat signal with a high degree of robustness to B0 field
inhomogeneity over conventional spectral saturation pulse techniques [2–5].
This work shows how the Dixon method can also improve upon the “out-of-phase” technique where the echo time is chosen so that fat is out of phase
in the acquired signal [6]. The proposed method also uses the spiral k-space
trajectory in [7] and its combination with the Dixon method as detailed in
[2] for application to time of flight (ToF) angiography in the head and neck.
The spiral acquisition technique improves the scan efficiency allowing the
acquisition of the three data points necessary for Dixon reconstruction while
improving upon the scan time of the conventional 3D multi-slab cartesian
ToF sequence.
Methods
Scan Parameters: The proposed method was compared to conventional
cartesian methods for 3D multi-slab imaging of the circle of Willis and 2D
multi-slice imaging of the carotid bifurcation. All scans were performed on
a volunteer using a 3T Philips Ingenia system with a 15 channel head coil.
3D ToF: The standard cartesian parameters used were: TR/TE = 23/3.5
msec, 16 x 16 cm field of view (FOV), 18˚ flip angle, a sampling window (tau)
of 5.7 msec and a partial echo acquisition of 65% in the readout direction for
a scan time of 5:25 min. The proposed spiral scan parameters were: TR =
21 msec, TEs = 1.24/1.99/2.74 msec, 24 x 24 cm FOV, 18˚ flip angle, tau =
7.2 msec, and 40 spiral interleaves per kz-encoding (fully sampled) for a scan
time of 4:02 min. Both sequences had a 1.4 mm slice thickness, 19 slices per
slab with an overlap of 9 slices for 5 slabs, flow compensation gradients and
a venous saturation pulse.
2D ToF: The cartesian scan parameters used were: TR/TE = 16/3.5
msec, 22 x 22 cm FOV, 30˚ flip angle, tau = 3.6 msec, and a partial echo
of 65%, for a scan time of 4:46 min. The proposed spiral scan parameters
were: TR = 25 msec, TEs = 2.5/3.25/4 msec, 35˚ flip angle, tau = 8.8 msec,
and 28 spiral interleaves per slice (fully sampled) for a scan time of 3:34 min.
The parameters used in both techniques were: 3 mm slice thickness with an
overlap of 1 mm, flow compensation and a venous saturation pulse.
Reconstruction: The reconstruction for the proposed 2D and 3D spiral
methods was implemented and processed in GPI [8]. In each reconstruction,
the three point Dixon method was used to calculate the B0 field maps. The
field maps are then used to reconstruct the three echo sets in a joint conjugate
gradient deblurring and water-fat separation [9].
Results & Discussion
The thin maximum intensity projection (MIP) images in figure 1 demonstrate that the removal of the fat signal allows for better visualization of the ophthalmic arteries, a region that can be significantly obfuscated by fat signal. Figure 2 shows how the fat signal in the orbitals and surrounding scalp
regions can come through in the full volume MIP images of the head. MIP
images of the carotid bifurcation (figure 3) show that fat signal is removed
from areas around the neck and posterior head.
Conclusion
This work has demonstrated the viability of using spiral and the three-point
Dixon method for water-fat separation in ToF angiography with a total scan
duration that is shorter than conventional methods. The authors believe
that the scan duration can be made substantially shorter by increasing the
sampling window duration as shown in [10].
Acknowledgements
No acknowledgement found.References
[1] A Grayev et al. “Improved time-of-flight magnetic resonance angiography with IDEAL water-fat separation”. In: Journal of Magnetic
Resonance Imaging 29.6 (2009), pp. 1367–1374.
[2] D Wang et al. “Analytical three-point Dixon method: With applications for spiral water–fat imaging”. In: Magnetic Resonance in
Medicine (2015).
[3] QS Xiang. “Two-point water-fat imaging with partially-opposed-phase (POP) acquisition: An asymmetric Dixon method”. In: Magnetic
resonance in medicine 56.3 (2006), pp. 572–584.
[4] J Berglund et al. “Three-point dixon method enables whole-body
water and fat imaging of obese subjects”. In: Magnetic Resonance in
Medicine 63.6 (2010), pp. 1659–1668.
[5] SB Reeder et al. “Iterative decomposition of water and fat with
echo asymmetry and least-squares estimation (IDEAL): application
with fast spin-echo imaging”. In: Magnetic resonance in medicine 54.3
(2005), pp. 636–644.
[6] QS Xiang and L An. “Water-fat imaging with direct phase
encoding”. In: Journal of Magnetic Resonance Imaging 7.6 (1997),
pp. 1002–1015.
[7] JG Pipe and NR Zwart. “Spiral trajectory design: A flexible numerical algorithm and base analytical equations”. In: Magnetic
Resonance in Medicine 71.1 (2014), pp. 278–285.
[8] NR Zwart and JG Pipe. “Graphical programming inter-
face: a development environment for MRI methods”. In: Magnetic Resonance in Medicine (2014).
[9] NR Zwart, D Wang, and JG Pipe. “Spiral CG deblurring and fat-water
separation using a multi-peak fat model”. In: Proceedings of the Joint
Annual Meeting of ISMRM-ESMRMB, Milan, Italy. 2014.
[10] CH Meyer et al. “Fast spiral coronary artery imaging”. In: Magnetic Resonance in Medicine 28.2 (1992), pp. 202–213.