Christoph Alexander Rettenmeier1 and V. Andrew Stenger2
1JABSOM, University of Hawai'i, Honolulu, HI, United States, 2University of Hawai'i, Honolulu, HI, United States
Synopsis
Phase offset multi-planar
(POMP) encoding is applied in a simultaneous multi-slice (NSMS = 4)
excitation scheme using half sinc pulses. In combination with a gradient echo
2D spiral readout trajectory and controlled aliasing in parallel imaging (CAIPI) via a model-based reconstruction a
fast ultra-short echo time (UTE) sequence is developed. Sequence details and
performance tests on short T2* phantoms are presented.
Introduction
UTE imaging enables the
visualization of short T2* tissue like ligament, white matter or cortical bone
that is not detectable with conventional MRI techniques. (1) In diseases such as
Alzheimer’s or multiple sclerosis crucial information on the pathogenesis may
be obtained from imaging these types of tissues. (2) Often half pulse
slice-selective excitation is used with a center-out readout to obtain a 2D
acquisition with a short TE. (3) However, challenges related to the fast signal decay
due to the short transversal relaxation time (T2) of the tissue of interest make
it difficult to obtain images of sufficient quality for clinical application in
a reasonable time frame. Furthermore the use of half pulse excitation requires
the summation of two pulses with opposite gradient polarity for slice
selection. In this work we propose to
decrease the acquisition time of the UTE half pulse method using simultaneous
multi-slice (SMS) methods. While SMS imaging has found widespread application
in combination with conventional slice-selective sinc pulses, UTE imaging using
half pulses has not benefited from it so far partially due to the need of phase
encoding gradients for optimal CAIPI sampling. Here we describe a UTE SMS
approach using POMP encoding in combination with a CAIPI under-sampling pattern
using spiral trajectories that are compatible with the requirements of short
TEs in UTE sequences.(4,5)Methods
NSMS = 4 SMS half pulses were
designed using the small tip angle approximation. Each individual slice was
given a different phase to obtain the phase pattern corresponding to one plane
in kz-space according to the POMP encoding. A total of four pairs of different
half pulses were designed. Figure 1 shows the pulses including the excitation
profiles including the phase encoding scheme obtained using Block equation
simulations in Matlab (Mathworks, Natick, MA). MRI measurements were
performed on a Siemens MAGNETON Prisma 3T (Erlangen, Germany) scanner equipped
with a 52-channel head coil. Data were acquired using a gradient echo (NEcho=2) 2D spiral trajectory (Ntot=32) over
22 cm FOV with a 128x128 matrix size, TE of 30 μs and 2.2 ms, TR of 400 ms and
gradient spoiling. The final images were obtained using a generalized
reconstruction method. The spiral acquisition was retrospectively
undersampled such that each pair of half pulses used a subset of the
interleaves forming a rotated spiral for an R=1, 2 and 4 CAIPI style
acquisition. The k-space trajectories and data were inserted directly into the
signal equation and solved numerically using a non-uniform Fast Fourier
Transform within a regularized conjugate gradient algorithm.(6,7) No coil
sensitivity information was used for acceleration. All reconstructions were
performed offline using Matlab. The sequence was tested on a phantom containing
differently concentrated aqueous MnCl2 solutions (up to 200 mM).Results
The POMP UTE sequence was tested on a short T2 phantom and compared to a corresponding single slice UTE sequence (figure 4). During the iterative reconstruction the simultaneously excited slices were quickly separated and no significant slice-cross-talk could be observed after 20 iterations. The fully sampled images (R=1) are comparable to those of the single slice acquisition. Even with an undersampling factor of R=2 no significant loss of image quality occurs, however, with R=4 artifacts become more pronounced. Conclusion
In conclusion the use of POMP and SMS provides a potential means for increasing speed for half pulse UTE acquisitions. In this example no coil sensitivity information was used and good slice separation was still observed. Further accelerations may be obtained using parallel imaging approaches.Acknowledgements
This project was supported by the NIH grants R01DA019912, R21EB02076, and K02DA020569.References
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