Denis Kokorin1, Jürgen Hennig1, and Maxim Zaitsev1
1Medical Physics, University Medical Center Freiburg, Freiburg, Germany
Synopsis
In this work, we discuss
off-resonance effects observed in zoomed DWI combined with 2D pulses
based on EPI trajectories. Our main focus is placed on the use of
parallel excitation (PEX) for shortening 2D pulses and further
minimizing the distortion. Experimental data were obtained using a 3T
MRI system with an 8-channel TxArray extension and analyzed in
detail. We conclude that the use of PEX improves the matching between
excitation and acquisition in zoomed EPI applications.
Introduction
Excitation of slice
profiles with a limited FOV was shown to be advantageous for
distortion reduction in zoomed EPI applications such as DWI [1-4].
Profile selection is accomplished normally by 2D pulses based on EPI
excitation trajectories [3,4]. However, due to long durations, 2D
pulses are sensitive to B0 deviations, manifesting themselves as
distortions in the excited profile [5]. In this study, we analyze
off-resonance effects observed in SE-EPI combined with 2D pulses. The
main focus is placed on new opportunities brought by parallel
excitation (PEX, [5-7]) for shortening 2D pulses and further
minimizing the distortion.
Theory
The thickness of a
designed slice is usually encoded either along the phase encoding
(PE) or frequency encoding (FE) directions of the excitation
trajectory (Fig. 1). In PEX, the trajectories are undersampled by
skipping lines and the resulting excitation replicates are suppressed
by using the B1 sensitivities during pulse design [6,7]. When FE is
along the slice selection direction (Fig. 1A), the PE gradients of
excitation and acquisition are applied in the same directions in
SE-EPI (Fig. 2A). Therefore, excitation and acquisition distortions
are observed along the same spatial dimension and combined with each
other in the final image. In another encoding scheme (Fig. 1B), the
excitation and acquisition PE gradients are in orthogonal dimensions
(Fig. 2B). Thus, strong field deviations might shift the profile
outside the refocusing position during excitation, resulting in an
SNR decrease during the EPI readout. PEX allows shortening of the 2D
pulses and thus reduces these effects in both techniques in Fig. 2.
Materials and Methods
Experiments were carried
out on a 3T MR scanner (Siemens Magnetom Trio) with an 8-channel
TxArray extension. The scanned object was a container filled with
water and plastic tubes. 2D PEX was exploited for both techniques in
Fig. 1 and 2. The RF pulses were designed using the small-tip-angle
algorithm combined with conjugate gradient optimization to
incorporate B1 data [8]. The excitation trajectories with slice
selection in the PE direction were defined over an FOE of 38.4×24 cm2
with a grid size of 192×16. The trajectories with FE along the slice
selection direction had an FOE of 38.4×9.6 cm2 and 32×32 samples.
Both trajectories were undersampled by skipping every second k-space
line.
The selected profiles
were imaged using GRE, which reflected the excitation distortions.
Afterwards, SE-EPI methods (Fig. 2) were tested for varying shim
settings. For the sequence in Fig. 2A, imaging was in a sagittal
orientation for PE along the "anterior-posterior" and
"posterior-anterior" directions, which corresponded to opposite
polarities of the PE acquisition gradients. The imaging in Fig. 2B
was in a coronal orientation.
Results
For default shim settings
(Fig. 3A), the profiles exhibited no visible distortions, when FE of
the pulses was along the slice selection direction. After the shim
currents were modified and scanning was repeated, stronger B0
deviations led to shearing of the profiles (Fig. 3B, C). The
distortion during excitation for the accelerated pulse was weaker
compared to the fully-sampled counterpart as shown in the GRE images.
The profiles underwent further distortions in EPI and appeared to be
sheared dramatically when PE was "anterior-posterior". For PE
along the "posterior-anterior" direction, the observed distortion
was minimal.
For excitation of
profiles with slice selection in the PE direction and default shim
settings, the observed distortions were also minimal (Fig. 4A). After
the resonance frequency was changed by 100 Hz, the selected slices
were shifted from the original position, resulting in a signal
decrease in EPI (Fig. 4B,C). However, the signal was partially
restored for the accelerated pulse due to its shorter duration.
Conclusions
PEX allows for a more
robust selection of limited profiles against off-resonance effects.
For the imaging scheme with slice selection along the FE dimension,
PEX offers additional degrees of freedom, in order to better confine
the FOV to the targeted organ in SE-EPI and DWI. For slice selection
in the PE direction, PEX makes DWI more robust again signal loss.
Acknowledgements
The
authors thank Dr. Kelvin Layton for helpful discussions.
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