Hyunyeol Lee1,2, Jing Xu2, and Felix W Wehrli2
1School of Electronics Engineering, Kyungpook National University, Daegu, Korea, Republic of, 2Department of Radiology, University of Pennsylvania, Philadelphia, PA, United States
Synopsis
Keywords: Quantitative Imaging, Metabolism
In the original qBOLD, it is challenging to separate deoxyhemoglobin’s
contribution to R
2' from other sources modulating the voxel signal. Further, extracting DBV and Y
v from measured R
2' is a nontrivial task. It was recently shown that the constrained qBOLD method was able to properly
separate the several confounding factors, yielding the expected contrast for
both Y
v and DBV maps across the entire brain, and, together with a
separate measurement of CBF, leading to whole-brain 3D CMRO
2 maps within physiologically plausible
ranges. Here, we validated the new 3D qBOLD
method with respect to repeatability and hypercapnic gas breathing challenges.
Introduction
Quantitative BOLD (qBOLD)1,2 allows evaluation of oxidative metabolism of the brain in the
resting-state by quantifying deoxygenated blood volume (DBV) and hemoglobin
oxygen saturation level of venous blood (Yv), based on measurements
of RF-reversible transverse relaxation rate constant R2′. However,
it is challenging in the original qBOLD to separate deoxyhemoglobin’s
contribution to R2′ from other sources modulating the voxel signal, for
instance, R2, R2′ from non-heme iron (R2,nh′), and macroscopic magnetic field inhomogeneities (ΔB0). Furthermore, the
qBOLD model is highly sensitive to noise, resulting in unstable estimation of DBV
and Yv, even with an accurate measurement of the heme-originated R2′ (R2,h′)3. To address these issues, we had previously introduced
a prior-constrained qBOLD method4 in which a plurality of
preliminary parametric maps (R2,
R2′, ΔB0, voxel
susceptibility (Δχ),
and cerebral venous blood volume (CBVv)) are constrained in the
qBOLD model. In that work it was shown that the method was able to properly separate
the above-mentioned confounders, yielding the expected contrast for both Yv and
DBV maps across the entire brain5, and, together with a separate
measurement of cerebral blood flow (CBF), leading to whole-brain 3D cerebral
metabolic rate of oxygen (CMRO2) maps within physiologically plausible ranges4.
The purpose of the present work was to validate the new 3D qBOLD method with respect
to repeatability and hypercapnic gas breathing challenges. Methods
Summary of constrained qBOLD: The qBOLD protocol in this study consists of
two in-house developed pulse sequences: alternating unbalanced SSFP-FID and
SSFP-ECHO (AUSFIDE)5 (Fig. 1a) and velocity-selective
venous-spin-labeling (VS-VSL)6 (Fig. 1b), yielding voxelwise maps of
3D R2, R2′, ΔB0, Δχ (Figs. 1c,
1d) and a volumetric map of CBVv
(Fig. 1e), respectively. In the qBOLD processing step, the AUSIFDE-derived
parameters serve as prior information in solving the following constrained
optimization problem:
$$\arg min_{\mathbf{\Theta}}\sum_{TE}|\mathbf{y}(TE)-\Xi (\mathbf{\Theta},TE))|^{2}+w|\Delta \chi -\Psi (\mathbf{\Theta})|^{2}+p|{{R_{2}}'}-\Upsilon (\mathbf{\Theta})|^{2}$$ [1]
where Θ={Yv,DBV,R2′,χnb} is the set of unknown parameters (χnb: non-blood
susceptibility). Definitions for the models,
Ξ, Ψ, and Γ, along with sub-parameters therein are
provided in Reference 4. In solving Eq. (1), VS-VSL-derived CBVv maps were used
to initialize and guide the solution of DBV. The regularization
parameters w and p were empirically determined.
Given the
estimates of Yv across the entire brain, oxygen extraction fraction (OEF) was
computed by OEF = 1-Yv/Ya with Ya = 0.98 (arterial blood oxygen saturation) assumed. Finally, 3D
pseudo-continuous arterial spin labeling (pCASL) with stack-of-spirals readout7
was employed for CBF mapping, leading to the derivation of CMRO2 by:
CMRO2=Ca·CBF·Ya·OEF where Ca
is the oxygen carrying capacity of arterial blood, obtained by scaling a
hematocrit level.
Experiments & analyses: All experiments were
performed at 3T (Siemens Prisma). To evaluate the present method’s
reproducibility, data were collected twice in seven healthy volunteers using the
three pulse sequences (AUSFIDE, VS-VSL, and pCASL). In all study subjects, the
second scans took place within two weeks apart from the first one. Additionally,
high-resolution T1-weighted images were also acquired for brain segmentation.
See Reference 4 for imaging parameters and data processing details. Both DBV
and OEF maps in a representative subject were presented for the two scans.
Furthermore, the interscan agreement of the two parameters in gray-matter (GM) was
evaluated using box plots and paired t-tests.
The same protocol was also applied in 11 healthy participants
under baseline and hypercapnic states, respectively, for further validation of
the technique. Here, the RespirAct system (Thornhill Research) was used to
target +8 mmHg of end-tidal partial
pressure of CO2 from baseline (equivalent to about 6% inspired CO2).
Following data processing, whole-brain 3D maps of CBF, DBV, OEF, and CMRO2
were obtained in a representative subject at baseline and hypercapnia. Thereafter,
GM averages of the four parameters across the 11 study subjects were compared
between the two states using paired t-tests. Results
Figure 2 displays test/retest whole-brain 3D maps of DBV and
OEF in the three orthogonal planes in a study subject. In both scans, DBV
images highlight the expected gray/white matter contrast while OEF values are
largely invariable across the entire brain, being consistent with the results
in our previous study4. Figure 3 shows box plots of GM averages of
DBV and OEF in the seven subjects. Paired t-test suggests that the test-retest
difference in both DBV and OEF quantifications is not statistically
significant.
Figure 4
shows parametric maps of CBF, DBV, OEF and CMRO2 reformatted into
the three orthogonal planes, obtained in a subject breathing
normoxic/normocapnic and hypercapnic gas mixtures. Box plots of GM averages of
the four parameters in the two states are shown in Fig. 5. Statistical comparisons
reveal that the hypercapnia-induced increases of both CBF and DBV and decrease
of OEF were all significant, whereas the CMRO2 changes due to the
hypercapnic stimulus were nonsignificant. Discussion and Conclusions
We evaluated the
performance of the constrained qBOLD based oximetric technique by examining its
repeatability and detectability on physiologic changes resulting from external
stimuli. Results suggest that the method yields the expected contrast across
the brain regions (GM vs. WM), across the measurement times (test vs. retest),
and further across the brain states (baseline vs. hypercapnia), albeit so far in healthy subjects. Clinical
validation in patients with neurovascular disease, for example, arterial steno-occlusive disease is forthcoming. Acknowledgements
NIH grants P41-EB029460 and R21-EB031364, and NRF Korea grant 2021R1F1A1045621References
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