Michael Carl1, Yajun Ma2, Graeme M Bydder2, and Jiang Du2
1Global MR Applications & Workflow, General Electric, San Diego, CA, United States, 2University of California San Diego, San Diego, CA, United States
Synopsis
Due to the fast decay rate of the transverse
magnetization, diffusion weighting is challenging in short T2 tissues; only
very limited b-values can be achieved before the signal decays to zero. In this
work, we used stimulated echoes to allow spin diffusion while the magnetization
is stored along the longitudinal axis, therefore achieving useful b-values and
allowing examination of short T2 tissues. Several technical challenges have to
be addressed however, such as minimizing the oscillatory signal banding due to
the low diffusion gradient area and reducing T1 contamination in multi-spoke UTE
acquisition. This initial proof-of-principle study shows good quantitative
agreement with clinical EPI diffusion sequences.Introduction
Imaging the very short
T2 tissues frequently encountered in the musculoskeletal system using MRI
requires specialized pulse sequences with very short echo times (TE). To
address this challenge, ultrashort TE (UTE) sequences such as 3DCones [1] typically
begin data acquisition as soon as possible after the RF excitation and acquire
k-space in a center out fashion [2]. Due to the fast decay rate of the
transverse magnetization, diffusion weighting is challenging in short T2
tissues. Only very limited b-values can be achieved before the signal has decayed
to zero. In this work, we used stimulated echoes to allow spin diffusion while
the magnetization was stored along the longitudinal axis, therefore achieving useful
b-values. We show that the technical challenges associated with this approach
can be overcome and that useful diffusion weighting can be achieved in tissues
with very short T2s.
Theory
The pulse sequence is shown in Fig.1. The
diffusion preparation module is repeated every TR period, and is immediately
followed by N separate k-space spokes during short time intervals τ. The
diffusion duration πΏ is kept sufficiently
small (1-5ms) to minimize T2 decay, while the main evolution time π₯ is chosen large enough (30-100ms) to allow
maximum b-values of 100 s/mm
2 or greater. Several challenges arise with this
approach: The first challenge using stimulated echo diffusion preparation with
small diffusion gradient areas is that the corresponding phase labeling
oscillation wavelength in the diffusion direction can be larger than the pixel
dimension and therefore appear as banding in the image (see Fig.2). The
wavelength of these oscillations is given by: π=2π/(πΎπΏG). In typical diffusion sequences the value of
πΏG is large and these oscillations do not
artifact the image. The most straightforward way to mitigate this issue is to
apply the diffusion gradients along the largest pixel direction which is
typically the slice direction. The second challenge is scan time. To minimize
the scan time, several k-space spokes can be acquired after each diffusion
preparation. However this causes T1 recovery contamination (especially for the
later spokes), so that the signals are artificially elevated for higher
b-values, resulting in an underestimation of D. One possible solution to this
problem is to reverse the phase of the second 90º pulse (see Fig.1) so that the magnetization is stored along the
negative z-axis. This results in an underestimation of the signals due to T1
recovery. Finally, phase cycling the second 90º pulse and averaging the acquisitions helps to offset these effects.
Methods
Bloch simulations were performed to study the
signal behavior and quantitative accuracy of the diffusion measurements. Phantom
scans were performed in a doped water phantom with T1/T2 = 100ms/65ms using a T/R head coil on a 3T GE HDxt
clinical MR scanner. The first scans
were performed with the diffusion gradient applied within the imaging plane to
highlight the confounding oscillation patterns for low b-values. Next, multi
b-value measurements were performed in the slice direction, with the diffusion
gradient area large enough so that several phase labeling cycles are contained within a slice (π << slice) at b-values from 0-100 s/mm
2. Three separate
acquisitions were performed, with the second 90º pulse chosen to either tip up the
transverse magnetization, tip down the transverse magnetization, or cycle
between both modes.
Results
Fig.2 shows two axial phantom images using
different small diffusion gradient areas applied left/right. The left image shows
the result with π
= 9mm, while the right one shows the result with π = 46mm. Figs.3A-C shows the simulated
signal decay curves as a function of b-value. Fig.3D shows the experimental results.
The data shown in blue is acquired so that the diffusion prepared magnetization
is stored along the positive z-axis before UTE imaging (resulting in higher
signals), while the data in red was acquired so that it is stored along the
negative z-axis (resulting in lower signals). Finally, the data shown in black
is the cycled data which converges to the signal levels of the clinical EPI
reference sequence (green).
Conclusion
Stimulated echo based
diffusion weighted 3DUTE MR imaging can be used effectively to achieve useful
b-values in short T2 MSK tissues. Several technical challenges have to be
addressed however, such as minimizing the oscillatory signal banding due to the
low diffusion gradient area, and reducing T1 contamination in multi-spoke UTE
acquisitions. This initial proof-of-principle study shows that this can be accomplished
and that good quantitative agreement with clinical EPI diffusion sequences is
possible.
Acknowledgements
No acknowledgement found.References
[1] Rahmer et al. MRM 55:1075–1082
(2006), [2] Gurney et al. MRM 55:575-582 (2006)