Qingjia Bao1, Eddy Solomon1, Gilad Liberman1, Samuel Cousin1, and Lucio Fydman1
1Department of Chemical and Biological Physics, Weizmann Institute of Science, Rehovot, Israel
Synopsis
SPatiotemporal ENcoding (SPEN)
provides single-shot 2D images free from T2* effects, and with enhanced
robustness to field distortions. SPEN’s acquisition module is relatively short,
opening the possibility to combine SPEN with a multi-spin-echo protocol, thus collecting
several images in one shot. This work explores this possibility towards two
different aims: the single-shot characterization of spatially-resolved T2 maps,
and the accelerated acquisition of 3D images incorporating a phase
encoding. Both approaches proved
successful, as exemplified with real-time T2 mapping of in vivo kidney
on a perfused mouse and high resolution volumetric acquisitions on ex vivo
phantoms and human volunteers.
INTRODUCTION
T2, T2* and quantitative
susceptibility mapping are valuable techniques [1-4], but their execution may
involve long scan durations, and thereby be affected by motion- or flow-induced
artifacts. SPatio-temporal ENcoding (SPEN) is a single-shot
technique that has been introduced as a complement to EPI, and which could
shorten these experiments [5]. Thanks to its reliance on a direct spatial acquisition
that is free from traditional Nyquist criteria, SPEN enables the use of strong
gradients along the low-bandwidth dimension. This can help overcome image distortions
arising from B0-or shift heterogeneities [6]; it can also produce improved
an image’s resolution by relying on restricted FOVs free from aliasing
artifacts. The relatively short sampling duration of SPEN experiments, usually shorter
than T2, opens the possibility of combining these advantages with the
incorporation of an additional modulating variable, by means of Multi-Spin-Echo
(MSE) approaches. This study presents the advantages resulting from doing so in
both preclinical and clinical settings. Specific
opportunities that are here discussed include (i) quantitative single-shot T2
mappings of phantoms and of a human brain; (ii) the real-time monitoring of T2 changes
upon injection of contrast material into live mice, and (iii) the possibility
to use the MSEs for phase-encoding a slab-selection axis (z) to accelerate volumetric
SPEN acquisitions with 3D isotropic resolution.METHODS
Phantom and rodents experiments
were performed on an Agilent DD2® 7T/110mm scanner using a quadrature probe; human
scans were acquired at 3T using a Siemens TrioTIM® scanner and a 12-channel head
coil following suitable written consents.
The MSE SPEN sequence used in this study is shown
in Figure 1A, in a version where the spin-echoes are interspersed with optional
gradient blips along the slab-selecting (z) direction. Should these gradients
be absent, the sequence would still reflect in the magnitude of each echo the T2
decay (orange points in Fig.1B) –but not the T2* effects, as these are
refocused in a position dependent manner. This in turn enables accurate T2
mapping from the magnitude-mode MSE SPEN data. Alternatively, the phase encodings
derived from the alternating even/odd SPEN echoes due to the effects of the
blipped gradients, provide an opportunity to introduce an additional z phase-encoding
(PE), from which single-shot volumetric reconstruction is feasible as explained
in Fig. 1C.RESULTS
Figure 2A compares T2 values
arising in a phantom containing different Gd-DTPA concentrations, when mapped
by the new single-shot MSE-SPEN approach and by a conventional multi-shot
spin-echo test. The good agreement shown by this phantom is also reproduced by
results collected on an ex-vivo rat once acquired by multiscan SE and once by MSE-SPEN
(Fig.2B); shown in Fig.2C are MSE-SPEN results acquired on a healthy human
volunteer. The fast T2 mapping of the ensuing setting could be useful for
functional or perfusion settings. The latter scenario was investigated by
administering a contrast agent to a live anesthetized mouse, and using MSE-SPEN
to generate real-time 2D maps of the animal’s T2 changes. Figure 3 shows abdominal results observed
before and after the injection of GdDTPA. The animal’s kidneys evidence a strong
T2 shortening during the wash-in of the contrast bolus, and subsequent T2
lengthening with its washout. These dynamics were different for different regions,
with the kidney’s cortex exhibiting lower basal end-levels than its medulla.
Another possibility opened by MSEs,
includes accelerating the acquisition of 3D acquisitions. The number of SPEN acquisitions the MSEs
could generate in this manner was 7 in the preclinical and 3 in human scanners – insufficient
for digitizing a complete FOV with sufficient resolution. Figure 4 shows,
however how, in combination with partial-Fourier processing, MSE-SPEN could still
successfully accelerate 3D human acquisitions (despite a reliance on a ca. 20%
oversampling for each slab). Figure 5 shows the results of a slightly different
z-phase encoding approach applied to image a rat head. In this case the full
FOVz was targeted in each scan; this, with the acquisition of 5
echoes, allowed us to collect a 3D image with 200µm isotropic resolution in sixteen
shots (this time without partial FT). CONCLUSION
Single scan MSE-SPEN is a robust technique for accelerating
volumetric or parametric acquisitions, capable of producing parametric 2D maps
or delivering 3D volume images, in relatively short times. Minor modifications
of the sequences here presented can also be conceived for encoding T2*
information, for the single-shot mapping of fields, susceptibilities or
chemical shifts, or for real-time diffusivity/flow measurements. CAIPI-based schemes [7] in combination with
parallel receive acquisitions could also enable the execution of the multi-slab
experiments here presented in a single-shot.Acknowledgements
We are grateful to Dr. Amir
Seginer and Dr. Zhiyong Zhang for valuable discussions. Financial support from the Minerva Foundation (#712277),
the Kimmel Institute for Magnetic Resonance and the Perlman Family Foundation (Weizmann)
are gratefully acknowledged.References
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