Linh N N Le1, Gregory J Wheeler1, Thomas Christen2, Greg Zaharchuk3, and Audrey P Fan 1,4
1Biomedical Engineering, University of California, Davis, Davis, CA, United States, 2Grenoble Institute of Neuroscience, Grenoble, France, 3Radiology, Stanford University, Palo Alto, CA, United States, 4Neurology, University of California, Davis, Davis, CA, United States
Synopsis
We
compared two approaches of quantitative Blood-Oxygenation Level-Dependent
(qBOLD) and vascular MR Fingerprinting (vMRF) to map brain oxygenation from Gradient-Echo
Sampling of Free Induction Decay and Echo (GESFIDE) scans acquired during
normoxic, hyperoxic, and hypoxic gas breathing conditions. In 12 healthy
subjects, OEF calculated from qBOLD (qOEF) and OEF generated from vMRF (vOEF) were
inversely correlated to pulse oxygenation (SaO2) (p=0.032 and p=0.014,
respectively), indicating that qBOLD and vMRF are reliable methods for brain
oxygenation mapping.
Introduction
Brain
oxygenation measurements are important indicators for studies of brain
pathologies and physiology. Different MRI methods to measure brain oxygenation
(e.g., oxygen extraction fraction) have been proposed, but have not been
directly compared to each other. Quantitative BOLD (qBOLD) and Vascular magnetic
resonance fingerprinting (vMRF) represent promising approaches for mapping brain
oxygenation based on gradient and spin echo scans.1,5,7 This
study directly compares qBOLD and vMRF oxygenation methods in healthy, young
participants scanned at 3T across various oxygen inhalation conditions. Methods
Twelve
healthy volunteers (33±6 yo) were
scanned at 3.0 Tesla (MR 750, GE Healthcare, Waukesha, WI). The MR imaging
acquisition protocols for this study included Gradient-Echo Sampling of Free
Induction Decay and Echo (GESFIDE) imaging for oxygenation measurements and T1-weighted
imaging for structural information and registration. GESFIDE imaging parameters
were spin echo TESE/TR, 100/2000 ms; 40 TEs
between 5 and 130 ms; voxel size 1.5x1.5x2.5 mm3; 14 slices. GESFIDE
acquisitions (3.5 min / scan) were acquired while participants breathed hyperoxic
gas (100% O2), normal air (21% O2), and hypoxic gas (14% O2) using an in-house
gas delivery setup. GESFIDE was then aligned to T1-weighted scan to create gray
matter masks and define regions of interest.
In this study, we compared two modeling techniques
to quantify brain oxygenation qBOLD and VMRF from the same GESIDE datasets (Figure
1).
For vMRF, a dictionary of signal time-courses
was generated by performing biophysical simulations of brain microvasculature
with known susceptibility.8 The dictionary contained 64,000 signal time-courses
using 40 different values of cerebral blood volume (CBV; 0-25%), microvascular
vessel radii (R; 1-25 µm), and tissue oxygen saturation (SO2; 0-100%) in every possible
combination. The signal evolutions across all 40 TEs for each voxel was then
compared against this dictionary to find the single best fit using an iterative
inner product pattern matching algorithm. With the closest simulated signal
known, the CBV, R, and SO2 values associated with that best fit are assigned to
that voxel. This was repeated for every voxel in the brain to generate full
quantitative parameter maps. For a direct comparison of metrics to qBOLD, the
SO2 measurements acquired using vMRF were converted to OEF measurements using $$$OEF = \frac{SaO_{2} - SvO_{2}}{SaO_{2}}$$$. Here SvO2 stands for venous oxygen
saturation and represents the measurements obtained from vMRF for each voxel,
and SaO2 is the average arterial oxygen saturation recorded via pulse oximeter
throughout each scan.
For qBOLD modeling, R2′ was calculated by
using the Free Induction Decay (FID) denoted as regime A of signal evolution,
with decay rate of R2*A, and refocusing echoes (regime B) with decay rate R2*B:
$$$R_2′ = \frac{R_2^*A - R_2^*B}{2}$$$. GESFIDE data were motion corrected with
MCFLIRT and smoothed with a Gaussian kernel of (σ = 1.5mm) to eliminate the
effect of noisy voxels in FSL6. The data then were analyzed by
linear qBOLD model2, implemented in MATLAB, which applies a linear
fit of GESFIDE signal to the spin echo displacement time, τ > 15ms (total of
5 data points) as shown in Figure 2B. Deoxygenated Blood Volume (DBV) was then
estimated directly from the linear model; where DBV is the offset between the
linear intercept and the spin echo data. OEF was then calculated by known
constant of proportionality: $$$OEF = \frac{3\times R_2^{'}}{DBV \times \gamma \times 4 \times \pi \times \triangle \chi_{0} \times Hct \times B_{0}}$$$, with γ as the
proton gyromagnetic ratio, Δχ0 as the susceptibility difference between fully
oxygenated and deoxygenated red blood cells, Hct as hematocrit, and B0 as the
field strength.
All parameter maps from both vMRF and qBOLD were
then transformed into a standard reference space (Montreal Neurological
Institute (MNI) space)3, to create group-level average maps as shown
in Figure 1. A linear mixed effects model was used to assess the correlation
between OEF using the different methods and the changes in SO2 calculated from
vMRF and OEF generated from qBOLD during different gas conditions.
Results
Compared
to the normal air condition, Figure 3 shows changes in OEF during
hyperoxia, and hypoxia. There was a significant increase in OEF during hyperoxia (p=0.001 and p=0.026, respectively);
and slight opposite results for hypoxia in vMRF and qBOLD. The correlation between OEF from qBOLD (qOEF) and OEF from vMRF
(vOEF) in gray matter with a mixed-effect model indicates a trend toward
positive correlation between qOEF and vOEF across all subjects and conditions, as
shown in Figure 4. OEF in brain gray matter was inversely correlated with
increased arterial oxygen saturation, as measured by pulse oximetry for both
oxygenation imaging methods (p=0.032 for vMRF and p=0.014 for qBOLD). Discussion and Conclusion
The
finding of this study reveals that brain OEF measurements from both qBOLD and
vMRF provide sensitivity to physiological changes across oxygen inhalation
conditions. OEF values from vMRF were overestimated compared to literature
values and compared to qBOLD. However, OEF maps from vMRF showed higher
signal-to-noise ratio and more significant changes during different gas
conditions, potentially reflecting the robustness of fingerprint matching to
noise. Further studies may utilize these models to assess oxygenation changes in
neurovascular conditions such as vascular dementia. Acknowledgements
This study was supported
by NIH R00-NS102884.References
- Stone, A., and Blockley, N. A streamlined
acquisition for mapping baseline brain oxygenation using quantitative BOLD.
NeuroImage. 2017; 147:79-88
-
Cherukara, M., et al. Model-based Bayesian
inference of brain oxygenation using quantitative BOLD. NeuroImage. 2019
- Evans A., et al. IEEE-Nuclear Science
Symposium and Medical Imaging Conference. 1993; 1813-1817
- Yablonskiy, A., et al. Theory of NMR
signal behavior in magnetically homogeneous tissues: the static dephasing
regime. Magn. Reason. 1994; 32:749-763
- Yablonskiy, DA. Quantification of
Intrinsic Magnetic Susceptibility-Related Effects in a Tissue Matrix. Phantom
Study. Magn Reson Med. 1998; 39:417-428
- M. Jenkinson, et al. FSL. NeuroImage,
62:782-90, 2012
- Christen T, Pannetier NA, Ni WW, et
al. MR vascular fingerprinting: A new approach to compute cerebral blood
volume, mean vessel radius, and oxygenation maps in the human brain.
Neuroimage. 2014;89:262-270.
- Pannetier NA, Debacker CS, Mauconduit F, Christen T, Barbier EL. A Simulation Tool for Dynamic Contrast Enhanced MRI. PLoS ONE. 2013;8(3):e57636.