Lijing Xin1
1Centre d'Imagerie BioMédicale (CIBM) Ecole Polytechnique Fédérale de Lausanne (EPFL), Switzerland
Synopsis
Mobile macromolecules (MM)
present as broad resonances underlying sharp metabolite resonances in 1H
MR spectra at short to moderate TEs. The accurate estimation of MM is an important
prerequisite for reliable quantification of metabolites. This lecture covers up-to-date knowledge about MM, how to handle MM for MRS quantification,
and also some open questions.
Background
Performing localized 1H MRS measurement at short TE allows us to
attain high SNR with minimal signal loss from T2 relaxation and J-modulation of
coupled metabolites. We can therefore achieve neurochemical profiling including
a large number of metabolites. In short to moderate TE 1H MR spectra,
broad resonances are observed underlying sharp metabolite resonances, which
arise from mobile macromolecules (MM). These broad MM resonances demonstrate
short T1 and T2 relaxation properties, and low apparent diffusion coefficients.
They are likely composed of overlapping spectra (J-coupled multiplets) from
various amino acids within different cytosolic proteins(1). Since an inaccurate
estimation of MM spectrum may lead to potential systematic errors in
quantification of neurochemical profile, the contribution of this broad MM
spectrum should be carefully handled.Impact of TE, B0, brain tissue, age and disease on MM
MM spectrum is constituted of signals of amino acids that are
J-coupled spin systems, of which spectral pattern evolves with pulse sequence
parameters, such as TE and TM(STEAM). In this case, MM spectrum measured for
short TE spectra would not be the correct prior-knowledge for spectra acquired
at other TEs. Thus, reliable MRS quantification requires to take into account a
TE/TM specific MM spectrum.
The spectral linewidth of individual MM resonances is determined
by multiple factors, such as its T2, macroscopic and microscopic B0
inhomogeneities, multiplicity pattern of amino acids, relative shifts of
chemical shifts of amino acids within different proteins. Like other J-coupled
metabolites, with the increase of B0, spectral resolution could be improved for
multiplicity of amino acids, which has been observed for spectral regions of
1-1.8ppm when increasing B0 from 1.5 to 7T(2).
One may pose the question that whether MM differs within various brain
regions and tissues (white matter and grey matter). Several studies in human
brain attempted to investigate this question. In (3-5), authors found that some
MM components differ between white matter and grey matter in human brain. For
rodents, only minor regional and species (rat vs mouse) differences have been
found, which may due to the fact that rodent brains contain mainly grey matter.
In addition, age dependence was observed for MM in human brain(6) and rodent
brain(7), which could be ascribed to the age-related tissue content
change.
Moreover, MM itself may serve as a potential biomarker for certain
pathologies. Studies in brain tumors, stroke and multiple sclerosis have
observed alterations in MM but dominantly in mobile lipid, which can contribute
to brain tumor classification. Future studies are encouraged towards the
understanding of the origin of these changes in MM components and its role in
disease pathophysiology.
Taken together, many factors could affect the amplitude or pattern
of MM spectrum. Therefore, a comprehensive characterization of MM with the
sequence parameters used at the respective B0 and pathological state is an
important prerequisite for metabolite quantification and the discovery of
potential disease biomarker. MM estimation for MRS quantification
Two approaches are generally used:
1. Measuring
MM spectrum in vivo and incorporating it in the fitting prior-knowledge.
The measurement of metabolite-nulled MM spectra in vivo relies on
distinct characteristics of MM from metabolites, i.e. short T1 relaxation time
and low apparent diffusion coefficient. Metabolite-nulling by inversion
recovery(IR), either single IR or double IR, is generally used for MM
measurement with the following key steps:
-
Vary a range of TIs to determine the optimal TI with
minimal metabolite residuals.
- Acquire
spectra at this TI with a longer TE to determine the residual metabolites.
- Use
a short TR(in single IR experiment): improve temporal SNR and further
saturate metabolite signals.
- Measurement
within a relatively small VOI to insure the narrowest linewidth possible.
- Optimal
water and lipid suppression to avoid baseline distortion.
- Post-processing: frequency/phase
alignment, removal of residual metabolites (e.g. jMRUI: HLSVD, AMARES),
the procedure of residual removal should be proceed carefully to avoid
introducing variability in MM.
Moreover, when sufficient gradient strength is available,
diffusion weighted MRS is an alternative method to measure MM in combination
with IR(8). A better metabolites attenuation can be achieved with diffusion MRS
which does not require further post-processing for residual metabolites
removal.
2. Mathematical estimation of MM spectrum
MM spectrum can be parameterized by splines, or other lineshape
functions such as lorentzian, gaussian and voigt. However, overparameterization
should be taken care of. More importantly, such an approach that lack of
physical/chemical basis could not predict the modulation of MM spectral pattern
with TE or other parameters.
The direct simulation of MM spectrum is not applicable at present,
as the number of amino acids and their chemical-environmental information
within different proteins are still not completely available. Pioneer work from
Behar et al. identified chemical shifts and J-coupling constants of some amino
acids using 2D-COSY MRS in dialyzed brain cytosol(1). Recently, Borbáth et al. attempted
to use chemical information provided by Biological Magnetic Resonance Data Bank to generate chemical shift histograms as amino acid basis sets(9).
Future work towards this direction may provide a physical estimation of MM
spectrum.
Co-edited MM in GABA spectral editing
Gamma-aminobutyric
acid(GABA) detection is hampered by its low abundance and spectral overlap
with other intensive metabolites and MM. To achieve distinct measurement,
spectral editing can be used including J-difference editing (e.g. MEGA) and
multiple quantum filters. MEGA is the most common editing method used for GABA
editing. Due to limited spectral dispersion at B0<7T, when applying editing
pulse at 1.9ppm, the MM resonance at 1.7 ppm is often affected by this editing
pulse and its coupling partner at 3ppm gets refocused, and thus co-edited with
GABA leading to a GABA+ (GABA+MM) measurement at 3ppm. The potential
alterations in MM such as with different tissue composition, diseases or ages,
would lead to quantification issues for GABA.
MM
suppression scheme was proposed, one may apply editing pulse symmetrical around
1.7ppm (i.e. 1.9 and 1.5ppm)(10). Note that the suppression efficiency is very
sensitive to frequency drift during the acquisition. Another way to suppress
co-edited MM is to use inversion recovery, while this requires the knowledge of
T1 relaxation and suffers simultaneous GABA signal attenuation. Lastly, one can
use extend TE allowing to use a highly selective editing pulse(11).Acknowledgements
No acknowledgement found.References
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