Sophie Malaquin1, Eloïse Mougel1, Melissa Vincent1, and Julien Valette1
1Université Paris-Saclay, Commissariat à l'Energie Atomique et aux Energies Alternatives (CEA), Centre National de la Recherche Scientifique (CNRS), Molecular Imaging Research Center (MIRCen), Laboratoire des Maladies Neurodégénératives, Fontenay aux Roses, France
Synopsis
Diffusion-weighted NMR spectroscopy allows non-invasive
measurement of the diffusion properties of brain metabolites. Lactate is of
particular interest but has low concentration thus requiring the development of
new sequences to maximize signal-to-noise ratio. In this work, we compare a
reference stimulated echo sequence and two spin echo sequences using either a
broad pulse, or a selective polychromatic pulse suppressing J-modulation, by
measuring the signal attenuation as a function of diffusion-weighting. Suppression
of J-modulation with the polychromatic spin echo sequence leads to a
significant signal gain and a better precision in lactate signal attenuation.
Introduction
In vivo diffusion-weighted NMR spectroscopy (DW-MRS) allows
measuring metabolite diffusion properties in the brain, and therefore to derive
information about the microstructural environment they diffuse in. The low
lactate concentration, compared to other metabolites, makes this measurement
difficult and requires the development of new DW-MRS sequences maximizing
lactate signal to-noise ratio. We compare the signal attenuation as a function
of diffusion-weighting b, between a reference sequence (STE-LASER)1,
as used in most of our recent works, and
a spin echo sequence (SE-LASER) where the DW spin-echo part relies on a
polychromatic pulse refocusing only the resonances of interest, therefore
suppressing J-modulation on lactate resonance at 1.31 ppm.Methods
Four wild-type mice were scanned on an 11.7 T Bruker system
with a quadrature surface cryoprobe. The STE-LASER sequence (fig.1a) starts by
a diffusion-weighting stimulated echo block (three broad pulses, TESTE/TM=8.4/50
ms, δ/Δ=3/53.2 ms),
and is followed by a LASER adiabatic localization bock (TELASER=25
ms). The SE-LASER sequence consists of a diffusion-weighting spin echo block
(TESE=58.3 ms) with the same diffusion timing as the STE-LASER (δ/Δ=3/53.2 ms), followed
by the same LASER block (fig.1). The sequence starts with a 90° adiabatic
excitation pulse. For the refocusing,
the spin echo block uses either a broad pulse (to assess the sole benefit of
using a spin echo compared to a stimulated echo, fig.1b), or a polychromatic
pulse (fig.1c). This pulse is inspired from works by Shemesh et al.2,3 and
is designed using the Shinnar-Le Roux algorithm. Its advantage relies on its
high selectivity: by choosing carefully the 180° pulse bandwidth, we can target
only the resonances of interest. In this work, in order to simultaneously
measure the diffusion of lactate and of metabolites with specific cellular
compartmentation, we chose to excite NAA (neuronal marker) at 2.02 ppm,
myo-inositol (astrocytic marker) at 3.56 ppm and the CH3 lactate
group at 1.31 ppm, and to exclude the CH lactate group at 4.09 ppm which the CH3
group is coupled with. This allows for the suppression of the J-coupling
effect on the 1.31 ppm resonance at the echo (moreover, the J-coupling effect
during the LASER block is negligible since it consists in a CPMG refocusing
train). First, spectra were acquired in a 31.5 µL hippocampal voxel of interest
without diffusion-weighting (b= 0.02 ms/µm², 128 repeats) with the three
sequences (STE-LASER, broad pulse SE-LASER, polychromatic SE-LASER), for signal
comparison. Then, the spectra were acquired at six different b-values (b= 0.02,
3.02, 5, 10, 15 and 20 ms/µm², TR=2000 ms, 128 repeats), with the STE-LASER
sequence and the polychromatic SE-LASER sequence (the full set of measurements
was performed in each mouse during the same session). Spectra were analyzed
with LCModel4. Experimental macromolecule spectra were included in
LCModel basis-sets. Note that the polychromatic pulse was designed to also
refocus the macromolecule resonance at 0.9 ppm to feed LCModel with extra
information to reliably quantify macromolecule signal overlapping with lactate
at 1.31 ppm (fig.3b).Results and discussion
The use of a stimulated echo in the STE-LASER sequence
results in the loss of half of the signal compared to a spin echo. The broad
pulse SE-LASER sequence allows for partially recovering signal despite longer
TE (fig.2a), but only for singlets such as NAA, tCho and tCr, not for lactate. The
polychromatic SE-LASER sequence allows for a similar signal increase for NAA,
and a spectacular lactate signal gain (fig.2b). Comparison of signal
attenuation as measured with the reference STE-LASER sequence and the
polychromatic SE-LASER sequence confirms the interest of using the latter for
measuring lactate diffusion at high b: while mean signal attenuation is
comparable between both sequences (i.e. there is no apparent bias) (fig.3),
standard deviation on lactate signal attenuation as measured across the four
animals is consistently lower with the polychromatic SE-LASER sequence, in
particular at the highest b-values (fig.4).Conclusion
This work shows that J-modulation suppression provided by
the polychromatic SE-LASER sequence leads to a significant increase in lactate
signal intensity, in turn resulting in better precision up to higher b-values.
In the future, the comparison of lactate diffusion with NAA (neuronal
metabolite), and with myo-inositol (astroglial metabolite) may provide
information on lactate distribution in these cellular types (as tentatively
done previously5) leading to a better understanding of the lactate
shuttle6.Acknowledgements
This project has received funding from the European Research
Council (ERC) under the European Union’s Horizon 2020 research and innovation
programs (grant agreement n° 818266)References
1. Ligneul,
C., Palombo, M. and Valette, J. Metabolite diffusion up to very high b in
the mouse brain in vivo: Revisiting the potential correlation between
relaxation and diffusion properties. Magn. Reson. Med., 2017;77: 1390-1398.
2. Shemesh,
N., Rosenberg, J., Dumez, JN. et al. Metabolic properties in stroked rats
revealed by relaxation-enhanced magnetic resonance spectroscopy at ultrahigh
fields. Nat Commun 5, 2014; 4958.
3.
Provencher SW. Estimation of metabolite
concentrations from local-
ized in vivo proton NMR spectra. Magn
Reson Med 1993;30:672–679
Provencher SW. Estimation of metabolite
concentrations from local-
ized in vivo proton NMR spectra. Magn
Reson Med 1993;30:672–679
3. Shemesh
N, Rosenberg JT, Dumez JN, Grant SC, Frydman L. Distinguishing neuronal from
astrocytic subcellular microstructures using in vivo Double Diffusion Encoded
1H MRS at 21.1 T. PLoS One. 2017;12(10):e0185232.
4. Provencher SW. Estimation of
metabolite concentrations from localized in vivo proton NMR spectra. Magn Reson
Med 1993;30:672–679
5. Ligneul C,
Palombo M, Hernández-Garzón E, et al. Diffusion-weighted
magnetic resonance spectroscopy enables cell-specific monitoring of astrocyte
reactivity in vivo. Neuroimage. 2019 May 1;191:457-469.
6. Barros
LF, Weber B. CrossTalk proposal: an important astrocyte-to-neuron lactate
shuttle couples neuronal activity to glucose utilisation in the brain. J Physiol. 2018;596(3):347-350.