Andreas Pohlmann1, Jason M Millward1, Paula Ramos Delgado1, Daniel Marek2, Didier Wecker3, Ralph Wissmann3, Helmar Waiczies4, Thoralf Niendorf1,5, and Sonia Wacizies1
1Berlin Ultrahigh Field Facility (B.U.F.F.), Max Delbrueck Center for Molecular Medicine, Berlin, Germany, 2Bruker BioSpin AG, Fällanden, Switzerland, 3Bruker BioSpin MRI GmbH, Ettlingen, Germany, 4MRI TOOLs GmbH, Berlin, Germany, 5Experimental and Clinical Research Center (ECRC), a joint cooperation between the Charité Medical Faculty and the Max Delbrueck Center, Berlin, Germany
Synopsis
MRI using i.v.
administered fluorine-19 loaded nanoparticles (NPs) allows the tracking of inflammatory
cell migration. The inherently low SNR limits the precise localization of 19F-labeled
inflammatory cells, because large voxel sizes are needed to collect sufficient
signal. To overcome this, we show here the first use of a novel 19F cryogenic
quadrature RF surface probe at ultrahigh field to substantially boost SNR beyond
that of state-of-the-art room temperature RF coils, while facilitating the
acquisition of better spatially-resolved images within shorter scan times.
Purpose
Neuroinflammatory autoimmune
diseases such as multiple sclerosis involve an early recruitment of
inflammatory immune cells from the periphery into the central nervous system [1].
Previously we studied immune cell infiltration into brains of mice with
experimental autoimmune encephalomyelitis (EAE), the animal model of MS, using fluorine-19
(19F)-loaded nanoparticles (NPs). Nanoparticles are administered
intravenously (i.v.), and are taken up by inflammatory cells during their
migration from the systemic circulation into the brain [2]. We detected the 19F-labeled
cells in vivo using a room
temperature (RT) dual 19F and 1H radio frequency (RF) volume
resonator employing 3D imaging with isotropic spatial resolutions above 600µm to
overcome 19F signal-to-noise ratio (SNR) constraints [2]. This limited
the information on the precise location of 19F-labeled inflammatory
cells in the brain. To overcome this, we show here the first use of a new 19F
transceive cryogenic quadrature RF surface probe (CRP) at ultrahigh field to substantially
boost SNR beyond that of standard state-of-the-art RT coils, while facilitating
the acquisition of better spatially-resolved images within shorter scan times.Methods
Experiments were
performed on a 9.4T animal MR system (Bruker BioSpin, Germany). The transceive quadrature CRP tuned to 376 MHz was compared with the volume resonator (ID=16mm) used previously
[2]. SNR gain estimation: Using a 15ml-phantom
filled with 30% 2,2,2-trifluoroethanol (TFE) in water, we acquired an axial 2D-RARE
image (TR=3000ms, TE=42ms, ETL=8, FOV=20mm, matrix=96, NEX=8). B1-mapping: On the same phantom we
acquired 3D-SE images (TR=6000ms, TE=4.5ms, FOV=28x16x16mm3, matrix=91x52x52,
NEX=1) with nominal excitation flip angles (FA) of 60 and 120 degrees and
calculated the actual FA using the double-angle method. SNR vs number of 19F atoms: NMR tubes (ID=4mm) were
filled with different concentrations of 19F-loaded NPs (Z-average diameter=164nm), which were
prepared using perfluoro-15-crown-5-ether (PFCE, Fluorochem, UK) [3]. Each tube was placed below the CRP surface
leaving a 1mm gap. SNR was calculated in an axial 2D-RARE image (TR=3000ms, TE=21ms,
ETL=8, FOV=20x20mm2, matrix=96x96, NEX=1).
High-resolution brain image: Animal
experiments were carried out in accordance with the local Animal Welfare
Department. To induce EAE, SJL/J mice were immunized with proteolipid protein
peptide139-151, and assessed daily for neurological symptoms [4]. PFCE NPs (10µmol) were administrated daily to
EAE mice i.v. (D5-D9 following immunization). Mice were sacrificed on D10,
fixed in paraformaldehyde and prepared in 15-ml tubes for ex-vivo MRI. 3D-RARE protocols were used for 19F MRI (TR=800ms,
TE=4.9ms, FOV=28x16x16mm3, matrix=182x52x52, ETL=26, NEX=384) and a 1H
reference image (TR=1300ms, TE=39ms, FOV=30x20x20mm3, matrix=192x128x128,
ETL=16, NEX=3).Results
We first compared the
performance of the CRP with the RT coil by estimating SNR of TFE phantom images
acquired with both coils. The 19F CRP SNR gain was calculated by
dividing the SNR for several ROIs (at increasing distances to the CRP surface)
by the SNR of a large central ROI in the RT coil image (Fig. 1). Up to a depth
of 8.5 mm the CRP had a superior SNR to the RT coil. Peak SNR gain exceeded a
factor of 6. To investigate the SNR achieved as a function of the number of 19F
atoms for a fast 2D-RARE protocol, we performed several scans with the 19F
CRP using phantoms with varying concentrations of PFCE NPs (25mM-200mM) and
with varying slice thickness (400µm-2000µm). The smallest number of 19F
atoms per voxel measured (5.2×1015) resulted in an SNR of 18 (Fig.
2). B1-Mapping (Fig. 3) demonstrated the typical inhomogeneity of a surface
coil array, very similar to those reported for 1H cryoprobes [5]. The
significant flip angle variation must be compensated for by B1-correction in
order to allow quantitative 19F imaging (Fig. 3). Using a 3D-RARE protocol as
previously described [2], we next acquired 19F MR images of a fixed
EAE mouse brain using the CRP. In these measurements we increased the spatial
resolution from 400x400x400µm to 154x308x308µm. Preliminary results with this
newly designed 19F CRP show a superior delineation of the areas of
immune cell infiltration, especially within the myelinated regions of the
cerebellum (Fig. 4) when compared to previous images obtained with the RT 19F
volume resonator [2].Conclusion
We carried out first tests
and high spatially-resolved MR measurements to determine the performance and
feasibility of using a quadrature 19F CRP for application in future in vivo studies. An SNR gain exceeding 6
compared with a state-of-the-art room temperature 19F RF coil facilitated
the acquisition of better spatially-resolved images. Preliminary
results in ex-vivo mouse brain show
the superiority of the quadrature CRP to delineate intricate areas of immune
cell infiltration, thereby inspiring future in-vivo investigations in neuroinflammatory disease.Acknowledgements
This work was supported by a grant of the Deutsche Forschungsgemeinschaft (DFG) to Sonia Waiczies and Andreas Pohlmann.
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