Seyedmorteza Rohani Rankouhi1, Donghyun Hong1, and David G. Norris1,2
1Erwin L. Hahn Institute for Magnetic Resonance Imaging, Essen, Germany, 2Donders Institute for Brain, Cognition and Behavior, Nijmegen, Netherlands
Synopsis
MEGA
edited 3 ppm signal can be severely contaminated with macro-molecules. Using
two distinct acquisition methods of MASE-sLASER and MEGA-sLASER both at TE = 68
ms at 7T, we show the feasibility of macromolecule free estimation of GABA with
LCModel. The presence of GABA line at 2.28 ppm in the spectra acquired with
both techniques plays a crucial role for this.
Introduction
The J editing1
or MEGA editing2 method for measuring GABA has the danger of
coediting other J-coupled metabolites in the edited 3ppm signal. Any coupled
metabolite with a resonance frequency close to 1.89ppm which is inverted by the
editing pulse and has a coupling partner at 3ppm will contribute in the edited
3ppm signal. There are macro-molecules (MM) that satisfy this condition3,4
and hence MM signal is co-edited with GABA leading to the 3ppm edited signal
often being termed GABA+. We recently demonstrated that with the MASE-sLASER
sequence at TE=68 ms, it is possible to measure the GABA resonance at 2.28ppm
well separated from the neighboring Glutamate resonance at 2.35ppm at 7T5.
At the same TE, the MEGA editing method is frequently used as an efficient tool
to measure the GABA resonance at 3ppm. In this study, we use these two MRS
tools to explore the degree to which measured GABA concentrations obtained with
these two distinct methods are similar.Methods
Sequence implementation: MASE-sLASER
and MEGA-sLASER sequences were implemented as described previously5. Data
acquisition: In total, 7 healthy subjects (2 female; age 29.7±5.8 years) participated in this
study, with approval from the local ethics committee. In vivo scans were performed on a 7T system
(Magnetom 7T, SIEMENS Healthcare GmbH, Germany) with a 32 channel Rx and single
channel Tx head coil (Nova Medical, NY). An anatomical reference image was acquired
using 3D MPRAGE6. B0 shimming was performed using FASTESTMAP7.
Single voxel MRS data were collected from two
voxels of size 20x20x20mm3 positioned in predominantly GM and predominantly
WM regions in the occipital lobe (Figure1) of 7 healthy subjects using
MASE-sLASER (TR=4500ms,TEs=68ms,NEX=64,scan time=5:06mins) and MEGA-sLASER
(TR=4500ms,TE=68ms,NEX=64,scan time=5:06min). Data analysis: Data
were analyzed using LCModel8,9 JMRUI10 and MATLAB (version 2016b,Natick,MA).
For the MASE-sLASER data, the
basis set for the LCModel analysis consisted of twenty-one simulated
metabolites. For the MEGA-sLASER editing data, six edited metabolites were
modelled: GABA, Glu, Gln, NAA, NAAG, and
GSH were included in the basis set. Each edited spectral model was created by
subtracting a simulated MEGA-off spectrum from a simulated MEGA-on spectrum.Results
Figure1
shows examples of MEGA-sLASER and
MASE-sLASER spectra acquired at TE=68 ms from predominantly GM and WM voxels
of a healthy human brain (subject3) and the corresponding voxel positions.
Figure2 (left) shows the correlation
between GABA/tNAA of MEGA and GABA/tNAA of MASE acquisitions both estimated by
LCModel. In Figure2 (right), we show the best fit and the corresponding R squared of the GABA/tNAA
ratio relative to GM fraction for MASE-sLASER (blue) and MEGA-sLASER (orange)
acquisitions separately.Discussion
Our estimation of 3ppm MEGA edited GABA
with LCModel at 7T is MM free. There are two arguments supporting this
assertion. First, in our MEGA edited spectra, in addition to GABA at 3ppm,
GABA at 2.28ppm is also fully coedited. This is because the narrow bandwidth
editing pulse (BW=133Hz) does not invert the 2.28ppm line. Therefore, the GABA
line at 2.28ppm contributes in the MEGA edited spectra in the same fashion as
3ppm GABA line but with the important feature of lacking MM contamination.
Compared with 2.28ppm line measured with MASE-sLASER, the 2.28ppm line here
is not separated from the neighboring Glutamate. LCModel however will still
incorporate it to estimate the GABA signal. Second, the linear correlation
between the GABA/tNAA ratio measured with the MEGA-sLASER sequence and
GABA/tNAA ratio measured with MASE-sLASER sequence which are both estimated by
LCModel has the slope of about 1 (0.94) (Figure2, left). This shows a very
strong correlation between the two distinct methods to measure GABA when
LCModel is used.
The GABA ratio in pure GM relative to in
pure WM that is derived from intercepts of the best fits of MASE-sLASER and
MEGA-sLASER (Figure2, right) represent somewhat different values (1.78 for
MASE-sLASER and 2.69 for MEGA-sLASER). However, both values lie well in the
range of what has previously been reported in the literature11-15.
The ratio of 1.78 derived from MASE-sLASER technique in this study matches with
reports by Mikkelsen et al11 Geramita et al12, and Zhu et
al13. The ratio of 2.69 derived with the MEGA-sLASER technique in
this study matches with reports by Choi et al14 and Jensen et al15.
Conclusion: Using LCModel analysis we validated two fundamentally
distinct GABA measurement techniques namely MASE-sLASER and MEGA-sLASER at
TE=68ms against each other. The presence of the 2.28ppm line in the spectra
acquired with both techniques is shown to be crucial for estimating MM free
GABA with LCModel.Acknowledgements
This
work was funded by the Helmholtz Alliance ICEMED – Imaging and Curing
Environmental Metabolic Diseases, through the Initiative and Networking Fund of
the Helmholtz Association.References
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