Hyungseok Jang1, Yajun Ma1, Michael Carl2, Saeed Jerban1, Eric Y Chang1,3, and Jiang Du1
1Department of Radiology, University of California San Diego, San Diego, CA, United States, 2GE Healthcare, San Diego, CA, United States, 3Radiology Service, VA San Diego Healthcare System, San Diego, CA, United States
Synopsis
Use of fat saturation pulses with UTE sequences can
improve short T2 contrast and parameter estimation, but can reduce the short T2
signal due to the broad spectrum. Moreover, conventional two-/three-point Dixon-based
methods can misestimate fat contents due to the short T2* decay in UTE imaging.
In this study, we demonstrate feasibility and efficacy of a single point Dixon
method to suppress fat for morphological and quantitative UTE imaging. We
evaluate the proposed framework in in vivo
experiments in a clinical 3T MR system: morphological UTE imaging and UTE-T1
mapping in knee joints and UTE-bone imaging in a leg.
Introduction
Fat suppression techniques are widely used in many
MRI applications (e.g., MSK and abdominal imaging) to achieve better image
contrast with suppressed signal from adipose tissues. UTE imaging can also benefit
from fat suppression for morphological and quantitative imaging, but
unfortunately, conventional fat suppression methods are problematic since the tissues
with short T2* decay demonstrate a broad spectrum; thusly, fat-saturation
pulses may undesirably suppress these tissues’ signals in addition to those of
fat. Moreover, the regular two-/three-point Dixon methods do not consider water
signal decay, so the estimated fat and water signals can deviate. In this
study, we propose a fast, simple, and robust method to suppress fat signal for
morphological and quantitative UTE imaging utilizing a single-point Dixon
(1p-Dixon) approach. Methods
In the proposed method, 3D-Cones dual echo UTE imaging
is utilized to acquire two images at TE1(UTE) and TE2(GRE) in a rapid single
scan (Figure 1). The complex MR signal in the image at TE2 is directly
decomposed to fat and water components using the 1p-Dixon approach1,2 after correcting phase errors
caused by phase offset and B0 inhomogeneity. Then, fat suppression can be performed
by applying a scaling factor to the fat image and simply subtracting the estimated
fat image from the UTE image. The scaling factor is automatically found such
that error between the UTE image and the scaled sum of the fat and water images
is minimized. The following in vivo
experiments were performed with 4 healthy volunteers on 3T GE-MR750: (Experiment-1)
morphological UTE knee imaging with 35- and 36-year-old males, (Experiment-2)
UTE variable flip angle (VFA) T1 mapping on the knee of a 36-year-old male, and
(Experiment-3) UTE bone imaging on the lower leg of a 31-year-old male. Imaging
parameters for Experiment-1 were: GE 8-CH transmit/receive knee coil, FA=20
degrees, TE1/TE2/TR=32µs/2.7ms/20ms, readout BW=±125kHz, FOV=160x160x96mm3,
matrix size=256x256x32, scan time=3min 53sec. The same parameters were used for
Experiment-2 except for the following parameters: four scans performed with FA=5,
10, 20, or 30 degrees; TE1/TE2/TR=32µs/2.9ms/20ms. Experiment-3 was performed
with the same parameters as Experiment-1 except for: matrix size=160x160x24 and
scan time=1min 54sec. External field map acquisition was performed with an
in-plane resolution reduced by a factor of 2. Results
Figure 2 shows comparisons between 2p-Dixon and
1p-Dixon in Experiment-1. As demonstrated, the short T2* decay in water is
misinterpreted as the coexistence of fat and water signals with 2p-Dixon.
Therefore, the fat signal is misestimated in tissues containing short T2*
components, as clearly indicated in the zoomed-in images of Figure 2-c;
meanwhile, the 1p-Dixon based method does not show this misestimated fat
signal. Figure 3-a shows the comparison between the 1p-Dixon based method and
conventional fat saturation in Experiment-1. As shown in the zoomed-in images of
Figure 3-b, the proposed 1p-Dixon based approach shows strong signal intensity
in the quadriceps and in the patellar tendons, with less spatial variation in
the fat suppressed UTE image, while the UTE image with FatSat exhibits
gradually varying signals as indicated by red arrows. The pattern of signal
variation in the UTE image with fat-saturation shows high similarity to the estimated
water images at TE2 (2.7ms), where most of the short T2* signals already
decayed. This observation implies broad-spectrum short T2* components were
partially affected by the fat saturation pulse. For both subjects in Experiment-1,
the proposed 1p-Dixon was able to suppress fat and to clearly visualize the
tendons. The measured contrast-to-noise-ratio (CNR) for the quadriceps tendon
with respect to the adjacent adipose tissue was 16.0±1.6 or 10.9±2.1 in the
1p-Dixon method, and 4.6±1.0 or 2.6±1.0 in the fat-saturation for the two
subjects. The measured CNR for the patellar tendon with respect to the
infrapatellar fat pad was 26.8±1.3 or 24.1±4.1 in the 1p-Dixon method and
17.5±1.0 or 9.9±1.9 in the fat-saturation for the two subjects. Figure 4
demonstrates 1p-Dixon applied to quantitative VFA-UTE-T1 mapping (Experiment-2).
Without or with 1p-Dixon fat suppression, the estimated T1 was 633.83±50.06 or
685.96±58.99, respectively, for the patellar tendon (Figure 4-a), and
914.75±123.71 or 989.93±132.86, respectively, for the posterior cruciate
ligament (Figure 4-b). Figure 5 shows the UTE bone imaging with application of
1p-Dixon method (Experiment-3), where the proposed 1p-Dixon method drastically
reduced partial volume artifact and aliased signal from fat (yellow arrows). Discussion and Conclusion
The proposed 1p-Dixon-based fat suppression method is
fast and robust, and addresses problems with conventional 2p-Dixon or fat-saturation
for UTE imaging. This approach is simple and therefore very flexible for
incorporation into various types of UTE imaging schemes such as UTE-T2* mapping3,4, UTE-T1 mapping5,6, and UTE-magnetization
transfer imaging7,8. Acknowledgements
The authors acknowledge research support from GE Healthcare, NIH (1R21AR073496, R01AR068987, R01AR062581) and VA Clinical Science and Rehabilitation R&D Awards (I01CX001388 and I01RX002604).References
1. Ma J. A single-point
dixon technique for fat-suppressed fast 3D gradient-echo imaging with a
flexible echo time. J. Magn. Reson. Imaging 2008;27:881–890 doi:
10.1002/jmri.21281.
2. Yu H, Reeder SB, McKenzie CA, et al. Single acquisition
water-fat separation: Feasibility study for dynamic imaging. Magn. Reson. Med.
2006;55:413–422 doi: 10.1002/mrm.20771.
3. Du J, Diaz E, Carl M, Bae W, Chung CB, Bydder GM.
Ultrashort echo time imaging with bicomponent analysis. Magn Reson Med
2012;67:645–649 doi: 10.1002/mrm.23047.
4. Du J, Bydder GM. Qualitative and quantitative
ultrashort-TE MRI of cortical bone. NMR Biomed. 2013;26:489–506 doi:
10.1002/nbm.2906.
5. Chen J, Chang EY, Carl M, et al. Measurement of bound and
pore water T 1 relaxation times in cortical bone using
three-dimensional ultrashort echo time cones sequences. Magn. Reson. Med.
2017;77:2136–2145 doi: 10.1002/mrm.26292.
6. Ma Y-J, Lu X, Carl M, et al. Accurate T 1
mapping of short T 2 tissues using a three-dimensional ultrashort
echo time cones actual flip angle imaging-variable repetition time (3D
UTE-Cones AFI-VTR) method. Magn. Reson. Med. 2018;608:598–608 doi:
10.1002/mrm.27066.
7. Ma YJ, Shao H, Du J, Chang EY. Ultrashort echo time
magnetization transfer (UTE-MT) imaging and modeling: magic angle independent
biomarkers of tissue properties. NMR Biomed. 2016;29:1546–1552 doi:
10.1002/nbm.3609.
8. Ma YJ, Chang EY, Carl M, Du J. Quantitative magnetization
transfer ultrashort echo time imaging using a time-efficient 3D multispoke
Cones sequence. Magn. Reson. Med. 2018;79:692–700 doi: 10.1002/mrm.26716.