Sungtak Hong1 and Jun Shen1
1National Institute of Mental Health, National Institutes of Health, Bethesda, MD, United States
Synopsis
Keywords: Data Analysis, Spectroscopy
Numerical Monte Carlo analysis was performed to
quantify metabolite-metabolite correlations of spectral origin in
31P
MRS spectra acquired from human brain at both 3 and 7 Tesla without any
confounding biological correlations. Significant correlations were found for many
31P-containing metabolite pairs. In particular, the 3 and 7 Tesla
NAD
+-NADH correlations are significantly different because of the
field strength difference. These results demonstrate that it is necessary to
incorporate metabolite-metabolite correlations originating from spectral
overlap into statistical models that correlate MRS measurements with clinical
parameters when overlapping
31P signals are of clinical interest.
Introduction
In vivo 31P MRS has been widely used to
study brain disorders. However, there is severe spectral overlap in 31P
MRS spectra even at 7 Tesla (for example, spectral overlap among α-ATP, NAD+, NADH, and UDPG). Since spectral overlap per se can lead
to significant correlations between metabolites1 it is necessary to
incorporate correlations of spectral origin into statistical models for
correlating overlapping 31P MRS signals with clinical parameters. In
this work, Monte Carlo analysis was performed to systematically quantify
metabolite-metabolite correlations of spectral origin in 31P MRS
spectra in the absence of any confounding correlations of biological origins. The
effects of field strengths and background spectral baseline on metabolite-metabolite
correlations were also characterized in detail. Methods
In
vivo 31P MRS data In vivo data of five healthy participants for each
field strength were analyzed. The in vivo 31P MRS data were acquired
using Siemens Skyra 3 Tesla and Magnetom 7 Tesla scanners (Siemens Healthcare,
Erlangen, Germany) and home-built coil assemblies using a circular 31P
coil with 7.0 cm diameter as described previously2. Briefly, in vivo
31P MRS data acquisition used a pulse-acquire sequence. Relevant
parameters at 3 Tesla were: TR = 2 seconds; spectral width = 5 kHz; number of
acquisitions = 128; number of data points = 1024. Identical parameters were
used at 7 Tesla except that TR = 3 seconds.
Data processing and quantification The same data processing procedure was
applied for both field strengths. The first two data points in FID were set to
zero to suppress the baseline in 31P MRS spectrum3.
Subsequently, zero-filling, 1-Hz exponential line broadening, Fourier
transform, zero- and first-order phase corrections, and chemical shift
referencing (PCr was set at 0 ppm) were performed. All spectra were quantified
using an in-house developed fitting program4 implementing the linear
combination model fitting algorithm5. Spectral regions covering -20
to 1 ppm at 3 Tesla and -20 to 10 ppm at 7 Tesla, respectively, were quantified.
The downfield region at 3 Tesla was excluded2. All basis data were
numerically calculated with chemical shifts and coupling constants taken from
the literature6,7. UDPG was excluded in the basis data of 3 Tesla due
to its low sensitivity. The background spectral baseline was modeled as a
polynomial. For calculating absolute concentrations, total ATP (sum of α-, β-,
and γ-ATP) were used as an internal reference, assumed to be 9 mM8.
Monte
Carlo analysis of in vivo spectra Individually
fitted metabolites including spectral baseline were derived from linear
combination model fitting. Subsequently, two different datasets comprising metabolites
only and metabolites + baseline were generated. Lastly, noise with its level
derived from the corresponding in vivo spectrum was added. For each spectrum 2000
different noise realizations were used. Each spectrum was then fitted using the
linear combination model fitting program described in Data processing and
quantification.
Correlation
analysis Using concentrations of
individual metabolites from Monte Carlo analysis, Pearson’s correlation
coefficients were calculated to investigate the effect of field strength and
spectral baseline on metabolite-metabolite correlations. Results
Figure 1
shows representative 3 Tesla (left panel) and 7 Tesla (right panel) in vivo 31P
MRS spectra. Means and standard deviations of metabolite concentrations obtained
at both field strengths are listed in Table 1. Tables 2 and 3 show the mean
Pearson’s correlation coefficient matrices derived from Monte Carlo simulations
performed using in vivo 31P MRS data at 3 Tesla (n = 5) and 7 Tesla
(n = 5), respectively. Due to the severe spectral overlap between NAD+
and NADH, the Pearson’s correlation coefficient of the NAD+-NADH
pair at 3 Tesla is quite large (r = -0.73 ~ -0.75) with and without the
baseline. In comparison, the Pearson’s correlation coefficient for the NAD+-NADH
pair is markedly reduced at 7 Tesla (r = -0.56). While UDPG is detectable at 7
Tesla it has significant correlations with both NAD+ and NADH. The background
spectral baseline was found to have significant influence on certain
metabolite-metabolite correlations. For example, the Pearson’s correlation
coefficient of the PC-PE pair changed from -0.11 without the baseline to +0.15
with the baseline at 7 Tesla. Discussion
Compared to the crowded short echo time proton MRS
spectra there is generally a wide chemical shift dispersion in 31P
MRS spectra. To the best of our knowledge correlations originating from
spectral overlap in 31P MRS spectra have not been taken into account
when correlating overlapping 31P MRS signals with clinical
parameters. However, at magnetic field strength such as 3 Tesla there is
significant spectral overlap in the downfield region involving phosphoesters, Pi,
and the prominent membrane phosphate signal that is not well understood2.
Even at 7 Tesla there is severe spectral overlap involving α-ATP, NAD+, NADH, and UDPG. The results of this study showed that spectral
correlations can be significant for 31P MRS data and are affected by
both field strength and the background spectral baseline. Therefore,
correlations in 31P MRS data due to spectral overlap need to be
built into statistical models for clinical analysis.Acknowledgements
No acknowledgement found.References
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