Guglielmo Genovese1,2, Lydia Yahia Cherif1,2, Malgorzata Marjanska3, Edward J Auerbach3, Romain Valabrègue1,2, Itamar Ronen4, Stéphane Lehéricy1,2, and Francesca Branzoli1,2
1Brain and Spine Institute (ICM), Center for Neuroimaging Research (CENIR), Paris, France, 2Sorbonne Universités, UPMC Univ Paris 06 UMR S 1127, Inserm U 1127, CNRS UMR 7225, Paris, France, 3Center for Magnetic Resonance Research and Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 4C. J. Gorter Center for High Field MRI, Department of Radiology, Leiden University Medical Center, Leiden, Netherlands
Synopsis
Diffusion-weighted MR spectroscopy (DW-MRS)
allows disentanglement of different pathological mechanisms of brain tissue by
exploiting the specific compartmentation of metabolites in different cell types.
In this study, we estimated the reproducibility of metabolite diffusion
measures obtained using DW-sLASER and DW-STEAM sequences at 3T. The inter- and
intra-subject variability of the apparent diffusion coefficients (ADC) of the
three major metabolites, as well as the effect of the acquisition time on the
variance of these measures were calculated for both sequences in two brain regions.
Power calculations were performed to facilitate the choice of the optimal
protocol for specific clinical needs.
Purpose
Diffusion-weighted
MR Spectroscopy (DW-MRS) allows investigation of metabolic and microstructural
properties of healthy and pathological brain tissue by probing the diffusion of
several intra-cellular metabolites in vivo1,2. The choice of the proper
sequence to be employed in a DW-MRS study depends on several factors, including
an optimal compromise between signal-to-noise ratio (SNR), precision of
metabolite quantification, and need for specific diffusion-weighting parameters.
While spin-echo sequences
provide higher SNR for a given echo time (TE), DW-STEAM allows for long diffusion
times keeping short TE, and it has been
shown to better quantify diffusion of J-coupled metabolites3. In this study, we calculated the reproducibility
of the apparent diffusion coefficients (ADC) of total N-acetyl aspartate (tNAA),
total creatine (tCr) and choline compounds (tCho), measured at 3T with both DW-sLASER
and DW-STEAM sequences from two brain regions containing mostly white or grey
matter. Moreover, we investigated the variance of metabolite diffusion measures
as a function of different acquisition times, and provided power calculations useful
for planning clinical studies. Methods
Single-voxel
DW-sLASER and DW-STEAM sequences were implemented for a 3T whole-body Siemens Prisma
scanner equipped with a 64 channel receive head coil. DW-MRS data were acquired
in the corona radiata (CR) and in the posterior cingulate cortex (PCC) of 11
healthy volunteers using a VOI of 8 mL. Each subject was scanned 3 times, using
either DW-sLASER or DW-STEAM. For DW-sLASER, diffusion weighting was applied in
3 orthogonal directions with diffusion time ∆ = 60 ms, gradient pulse duration δ = 18 ms, and 3 b-values of 11, 850, 3300 s/mm2 (40 averages
per condition). For DW-STEAM, diffusion weighting was applied in one direction
with ∆ =
85 and 316 ms, δ = 9 ms, and gradients applied with both positive and negative
polarities to minimize cross-terms effects related to background gradients,
resulting in a b-value of 3300 s/mm2 (64 averages per condition). TE
was 120ms and 30ms for DW-sLASER and DW-STEAM, respectively. The TR was
synchronized with cardiac cycles using a pulse-oximeter device and optimized trigger
delay. For 2 subjects, partial data were acquired using different trigger delays
for optimization. Unsuppressed water data were acquired for eddy current
corrections. Phase and frequency corrections on individual spectra were
performed before summation. A threshold on tNAA signal intensity was applied to
eliminate spectra with low SNR. Metabolite ADCs were estimated from
mono-exponential fits of the signal decay induced by the diffusion weighting. LCModel4
was used for metabolite quantification. Metabolite ADCs
and their variability as a function of the acquisition time were investigated
varying the number of b-values and spectra utilized for analysis (315, 270, 225,
180 and 135). Re-sampling was performed using bootstrapping (150 iterations).
Power and coefficients of repeatability (CR) and variation (CV)
were calculated for all measures using standard procedures5.Results
Good quality spectra were obtained in the 2 VOIs
using both sequences (Fig. 1). The effect of spectral processing and trigger
delay at high b value is shown in Fig. 2: the number of discarded spectra after
peak thresholding increased drastically for a non-optimized trigger delay.
ADC(tNAA) calculated with and without peak thresholding from all subjects, all
sessions, and 3 directions are reported in Fig 3. The variability of the
measures was significantly smaller when a threshold on signal intensity was
applied and depended on the diffusion direction. Table1 reports, for each session, tNAA, tCr
and tCho ADCs, averaged over diffusion directions and subjects. The CR
for ADC(tNAA) measured with DW-sLASER was 0.04 mm2/ms (27%) for the full acquisition (14 min) and 0.05 (31%)
for the 2-b values acquisition (9 min). Preliminary DW-STEAM data acquired at
the shortest ∆ suggested comparable variance of the
measures. Power calculations performed for DW-sLASER full and partial data sets
suggested that a difference between groups of 10% for ADC(tNAA) in the CR can
be detected with groups of 16 or 20 subjects each, respectively (Fig. 4C). Mean
ADC(tNAA) and CV estimated for different number of scans in the CR
are reported in Figs. 4A and 4B. Similar results were obtained in the PCC (data not
shown).Discussion and conclusion
We reported an evaluation of the performance of
DW-sLASER sequence, showing acceptable reproducibility for ADC(tNAA) measures
in the CR and PCC, in line with a previous study6, and demonstrating the feasibility of
DW-MRS in clinical settings. The full
study will incorporate an exhaustive comparison between DW-sLASER and
DW-STEAM in terms of reproducibility of
the 3 major metabolite diffusion measures, sample size calculation, as well as
reproducibility of DW-STEAM measures acquired at a long diffusion time of 316 ms.Acknowledgements
The research leading
to these results received funding from the programs 'Institut des neurosciences
translationnelle' ANR-10-IAIHU-06 and 'Infrastructure d’avenir en Biologie
Santé' ANR-11-INBS-0006. MM acknowledges support of following NIH grants: BTRC
P41 EB015894, and P30 NS076408.References
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