Alexander Gussew1, Andreas Masek1, Martin Krämer1, and Jürgen R. Reichenbach1
1Medical Physics Group, Institute of Diagnostic and Interventional Radiology, Jena University Hospital - Friedrich Schiller University Jena, Jena, Germany
Synopsis
The
reliability of 1H-MRS MEGA-PRESS measurements of inhibitory neurotransmitter GABA in the human
brain typically suffers from macromolecular (MM) contaminations of GABA
resonances. In this work, we present a novel MM suppression approach, which relies
on adiabatic inversion of the longitudinal magnetization of both metabolites
and MMs prior to playing out the MEGA-PRESS editing scheme, which is applied
after an inversion time delay (TI) corresponding to the zero-crossing of MM
magnetization. As demonstrated in healthy subjects, this new approach ensures appropriate
MM suppression and provides additional GABA signal gain compared to the commonly
applied approach with symmetrical MM editing.
Purporse
MEGA-PRESS
1H-MRS measurements of inhibitory neurotransmitter GABA allow
investigations of neurochemical processes modulating neuronal activity in the
brain1. Applying a standard MEGA-PRESS sequence with alternating
editing pulses at 1.9 ppm (edited spectra, ed) and 7.5 ppm (non-edited spectra, ned), the GABA intensities at 3 ppm in the difference spectrum
(ed–ned) are, however, overlapped by co-edited
macromolecular resonances (MM), which vary depending on physiologic factors or
disease state. The MM resonances can be suppressed by alternating narrow-band editing
pulses at 1.9 ppm and 1.5 ppm, providing similar MM modulation in both
ed and ned spectra, whereas GABA will be edited only in ed scans (‘Henry method’2). The editing efficiency for MM (and also
for GABA) can, however, be compromised by gradient heating or movement related
rf frequency drifts. In this study, we present a novel MM suppression approach relying
on an adiabatic inversion of the longitudinal magnetization of both metabolites
and MMs prior to playing-out the standard MEGA-PRESS editing scheme, which is
applied after an inversion time delay (TI) corresponding to the zero-crossing
of the MM magnetization.
Material and Methods
A
conventional MEGA-PRESS sequence (Siemens IDEA, VE11B) was modified by
inserting a spatially non-selective, adiabatic inversion pulse (BIR4). The TI
time for MM nulling (TI0,MM(T1,MM) = T1,MM × ln(2)) was set to 0.173 s, according to the
previously reported T1 of 0.25 s for MM in the human brain3.
Six healthy males (32.5±5.8 years) were measured on a whole-body 3T MR
scanner (Magnetom PRISMA, 64-channel head-matrix coil). The protocol comprised
a 3D T1-weighted MP-RAGE scan, followed by three 1H-MEGA-PRESS
water-suppressed scans (TR: 4.5 s, 64 ned/ed averages) in the posterior cortex (PC, 18 ml, see Fig. 1).
The first scan was performed with a conventional editing scheme to determine
the MM contaminated GABA+ intensities (‘ConvMEGA’,
TE: 68 ms, Gaussian editing pulse duration: 17 ms), whereas the
second scan was conducted by using the Henry Method
to quantitate ‘pure’ GABA intensities (‘HenryMEGA’,
TE: 80ms, alternating editing pulses at 1.5 and 1.9 ppm, editing
pulse duration: 23ms). Finally, the novel MEGA-PRESS sequence with
adiabatic MM nulling was applied during the third scan (‘MMnulMEGA’, TE/TI: 68/173 ms, editing pulse duration: 17ms).
GABA+ (ConvMEGA) and GABA (HenryMEGA and MMnullMEGA) intensities were quantified from the particular
difference spectra (jMRUI4) and normalised with the creatine
intensities obtained from corresponding ned
spectra (GABA+/tCr, GABA/tCr and Glx/tCr ratios).
Results
Figs.1
and 2 show representative ned and
difference spectra acquired with HenryMEGA
(blue graphs), MMnulMEGA (red graphs)
and ConvMEGA (black graphs) scans. Due
to progressing signal recovery during the TI delay, the tNAA, tCr and tCho
resonances are distinctly lower in the MMnullMEGA
compared to the ConvMEGA spectrum. On
the other hand, the ned and
difference MMnullMEGA spectra yield
the most flat baseline between 0.5 and 1.9 ppm, which evidences appropriate
MM suppression. Similar to the MMnullMEGA
ned spectrum, the corresponding
difference spectrum reveals an apparent, T1-weighting related decrease
of the GABA and Glx peaks. The GABA peaks in the MMnulMEGA and HenryMEGA
difference spectra are lower than in the ConvMEGA
spectrum due to suppressed MM multiplet fraction. Interestingly, the MMnullMEGA GABA resonance is higher than
in the HenryMEGA spectrum, where the editing
at 1.5 ppm particularly co-edits GABA at 1.9 ppm, leading to a GABA signal
reduction in the difference spectrum. These method-specific GABA signal modifications
are also replicated in the GABA/tCr subject group distributions (Fig. 3). Fig. 4
shows associations between GABA and GABA+ intensities obtained in scans with
and without MM suppression. Considering the Henry
method to be the gold standard approach for pure GABA measurements, the significant
correlation between the MMnulMEGA and
HenryMEGA GABA levels (Fig. 4a) indicates
appropriate GABA quantitation with the novel MMnulMEGA method. On the other hand, the weaker associations
between the GABA+ (ConvGABA) and pure
GABA levels (MMnulMEGA or HenryMEGA, Fig. 4b) illustrate the GABA+
uncertainty arising due to inter-individually varying MM levels.
Discussion and Conclusion
We propose
a novel method, which combines MEGA-PRESS 1H-MRS with adiabatic MM
nulling and provides appropriate GABA quantitation without macromolecular
contaminations. Besides being less dependent on rf-frequency drifts, our method
avoids GABA co-editing and provides a GABA signal gain compared to the Henry method. In addition, our method allows
more flexible editing pulse frequency selection in ned scans, which can be exploited for advanced editing strategies
as they are applied, for example, in the HERMES approach5.
Acknowledgements
Alexander Gussew and Martin Krämer acknowledge
funding from the German Research Foundation (DFG, GU 1108/3-1; RE 1123/22-1). Andreas Masek is supported by
a graduate scholarship from the Friedrich‐Schiller‐University Jena
(Landesgraduiertenstipendium).
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