Mathieu David Santin1,2, Isabelle Plu3, Vincent Gras4, Michel Luong4, Edouard Chazel4, Franck Mauconduit4, Alexis Amadon4, Alexandre Vignaud4, Cecile Lerman4, and Nicolas Boulant4
1Institut du Cerveau – Paris Brain Institute – ICM, INSERM, CNRS, Sorbonne Université, Paris, France, 2CENIR - Centre for NeuroImaging Research, Sorbonne University, Paris, France, 3Hôpital Pitié-Salpêtrière, AP-HP, Paris, France, 4CEA, CNRS, BAOBAB, NeuroSpin, University of Paris-Saclay, Gif-sur-Yvette, France
Synopsis
Keywords: High-Field MRI, Quantitative Susceptibility mapping
This work presents the first QSM images obtained on the 11.7T whole body Iseult system, using tailored
parallel
transmission k
T-point
pulses and a virtual coil approach for coil combination, on a post mortem brain.
introduction
QSM
at ultra-high field presents strong benefits due to an enhancement of
the susceptibility effect [1]. However, B0
and B1
field inhomogeneity make full exploitation difficult. Here we show
the first QSM images obtained on an ex
vivo
brain and with the whole-body 11.7T Iseult magnet, using tailored
parallel transmission kT-point
pulses and a virtual coil approach for coil combination.Materials & Methods
Brain
extraction was approved by the national biomedicine agency (Agence de
la Biomédecine) and the French ministry of Health. The encephalon
was imaged using the 11.7T Iseult MRI with Siemens VE12U software. An
8/32-channel custom built pTX head coil was used for signal emission
and reception. Before imaging, the ex
vivo
brain was transferred to a vial containing Fluorinert (Sigma,
Germany) to decrease the magnetic susceptibility mismatch between the
samples and the buffer. MR images were acquired using a 3D Multi Echo
Gradient Echo sequence with an isotropic resolution of 700 µm.
Parameters were: FOV= 192*192*134 mm, Mtx= 280*280*192, TR = 30 ms,
TEs ranging from 2.00 to 23.44 ms with a ΔTE of 2.68 ms (9 echoes
acquired). Flip angle was 10° and only one Nex was acquired. A 2*2
GRAPPA scheme was used to speed up the acquisition, leading to a scan
time of 5 minutes 28 s. Flip angle homogenization was performed using
tailored parallel transmission kT-point
pulses [2] generated offline in Matlab (The Mathworks, NA, MA, USA)
following the acquisition of B0- and B1-maps. Raw data was saved for
further processing. Magnitude and Phase images were generated
offline and coil combination was performed using a Virtual Coil
approach [3] again using Matlab. Images of multiple echoes were
combined using a root mean square along time dimension, thus
providing both high SNR and T2*-contrasted images. Brain mask was
obtained using ITK-SNAP software and a combination of morphological
operations (closing and erosion). Transversal relaxation rate (R2*)
was evaluated using a nonlinear fitting method in Matlab.
Quantitative Susceptibility Mapping (QSM) images were reconstructed
using several functions from the MEDI Toolbox [4-5] for both
background field removal and dipole inversion, using respectively
Laplacian Boundary Value (LBV) and a GPU modified L1-MEDI function.Results
Figure 1 presents the images obtained from the ex
vivo
brain with and without the use of kT-point
pulses. B1 signal inhomogeneities are clearly seen on images without
kT-point
pulses and vanish using kT-point
pulses excitation. Figure 2 presents the images obtained for
anatomical T2*w - SWAN, R2* and susceptibility maps. Virtual coil
combination provided naturally unbiased magnitude images (no
normalization used). Moreover, no clear evidence of abnormal signal
inhomogeneity due to bad B1-shimming or coil combination were
identified on these images. Several air bubbles were identified on
R2* and susceptibility maps, thus giving raise to high susceptibility
values in these regions.Discussion & Conclusions
Here
we reported the first QSM images obtained at 11.7T on an ex
vivo
brain at 700µm isotropic resolution obtained in approximately 5
minutes. We showed the feasibility of using tailored kT-pulses
and virtual coil combination for providing R2* and susceptibility
maps using a limited resolution for ultra-high field strength. We now
intend to push further image resolution to detect details and
features that might not be visible at conventional field strength on
big samples. Degassing the sample before imaging will certainly limit
the presence of air bubbles within the vial and sample.Acknowledgements
No acknowledgement found.References
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