Hyunyeol Lee1,2, Jing Xu2, Maria A Fernandez-Seara2,3, 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, 3Department of Radiology, Clinica Universidad de Navarra, Pamplona, Spain
Synopsis
Keywords: Quantitative Imaging, Metabolism
Recent
advances of the cBOLD technique by means of dual-gas calibration have shown its ability
in producing baseline OEF and CMRO2 in absolute physiologic units. A recently proposed constrained qBOLD method has
shown its feasibility in proper separation of numerous confounders, yielding
physiologically plausible values for both Yv and DBV across the entire brain. The purpose of this work was to compare
the two oximetric techniques, dual-gas cBOLD versus constrained qBOLD, in terms
of measured OEF and CMRO2 at baseline. Results suggest that
the two methods yield statistically insignificant differences in OEF and CMRO2
quantifications for GM regions.
Introduction
Paramagnetism of deoxygenated hemoglobin (dHb) perturbs local
magnetic fields, thereby modulating the MR
signal, a well-known BOLD contrast mechanism. Thus, dHb concentration in the venous
blood ([dHb]v) and deoxygenated blood volume (DBV) are the two
critical determinants of the BOLD signal1,2. Calibrated BOLD (cBOLD)3
aims to find a calibration constant (termed ‘M’) incorporating the two
parameters by comparing the BOLD signal in two states of the brain – one at
baseline and one in an isometabolic (e.g., hypercapnia) state. While early
attempts4,5 were only able to yield relative changes of oxygen
extraction fraction (OEF) and cerebral metabolic rate of oxygen (CMRO2) in
response to neural stimulations, recent advances of the technique by means of dual-gas calibration have
shown its ability in producing baseline OEF and CMRO2 in absolute
physiologic units6,7.
Quantitative BOLD (qBOLD)8,9 is another class
of methods that does not require a gas breathing challenge, and thus is
calibration-free. The method models dHb-induced signal modulations in the
extravascular compartment, and seeks to quantify both [dHb]v (or
venous oxygen saturation Yv via [dHb]v = [Hb](1-Yv)) and DBV by
estimating the RF-reversible component of the transverse magnetization (i.e., R2′).
A key challenge in qBOLD is to
separate the contributions from the four mechanisms that affect the temporal signal decay: R2, R2′ from heme (R2,h′) and non-heme (R2,nh′) iron
contributions, and macroscopic magnetic field variations (ΔB0).
Furthermore, disentangling R2,h′ into Yv and DBV is a nontrivial
problem due to the parameters’ mutual coupling10. A recently proposed
constrained qBOLD method11 has shown its feasibility in proper
separation of the above-mentioned confounders, yielding physiologically
plausible values for both Yv and DBV across the entire brain.
The purpose of this work was to compare
the two oximetric techniques, dual-gas cBOLD versus constrained qBOLD, in terms
of measured OEF and CMRO2 at baseline. Methods
Data were acquired in 13 healthy subjects at 3T (Siemens
Prisma) using both dual-gas cBOLD and qBOLD protocols. The dual-gas cBOLD
protocol consists of three successive episodes – normocapnic/normoxic baseline
(6 min), hyperoxia (~ 50% inspired O2; 6min), and hypercapnia (~6% inspired
CO2; 6min). Target gas mixtures were administered to the subject via the
RespirAct system (Thornhill Research). In each episode, a recently introduced
pulse sequence (termed ‘OxBOLD’)12, comprising 3D stack-of-spirals
pCASL (for CBF mapping), T2*-weighted multi-slice 2D spiral (for BOLD imaging),
and dual-echo GRE (for Yv estimation at superior sagittal sinus (SSS))
acquisitions, was repeatedly applied (20 pairs of pCASL control/tag). See
Reference 12 for detailed sequence structure.
Baseline OEF mapping from the dual-gas cBOLD data was
performed by following the processing steps in Reference 6. Briefly, the
calibration parameter M was derived by comparing baseline and hypercapnic
CBF/BOLD signals, followed by OEF derivation using the determined M, and
baseline and hypercapnic CBF/BOLD images. Here, M-calibration was carried out
using two different approaches, based on: 1) Davis model4 assuming
isometabolism of the hypercapnic challenge, and 2) OxBOLD model12
measuring Yv of SSS without the isometabolic assumption in 1). Gray matter (GM)
averages of M obtained using the two models were statistically compared.
The qBOLD
protocol consists of three pulse sequences: alternating unbalanced SSFP-FID and
SSFP-ECHO (AUSFIDE; 8min)13 yielding a set of volumetric maps (R2, R2′, voxel
susceptibility, ΔB0), velocity-selective
venous-spin-labeling (VS-VSL; 3.3min)14 for 3D venous blood volume estimation, and 3D stack-of-spirals pCASL
(4.5min)15. Parametric maps obtained from AUSIFDE and VS-VSL data serve as prior
information in solving a constrained qBOLD problem11, leading to 3D
maps of Yv, DBV, and R2,nh′ across the entire brain. See Reference 11 for processing
details in the constrained qBOLD mapping. Given the measured Yv, OEF was
computed by OEF = 1-Yv/Ya with Ya = 0.98 (hemoglobin oxygen saturation
of arterial blood) assumed.
Given the baseline
OEF measurements along with pCASL-derived CBF, baseline CMRO2 maps were
computed in dual-gas cBOLD and qBOLD methods, respectively, using the Fick’s Principle
equation CMRO2=Ca·CBF·Ya·OEF (Ca: oxygen carrying capacity of
arterial blood). GM averages of OEF and CMRO2 across 13 study subjects were
compared using paired t-tests.Results
Figure 1 compares whole-brain 3D M maps in a subject,
obtained using the Davis and OxBOLD models. Figure 2 shows a corresponding
Bland-Altman plot for GM-averages in 13 subjects. Group-averaged M values, 8.0±2.5
(Davis) and 8.2±3.7 (OxBOLD), are not statistically different (p=0.8). Hence,
we chose the OxBOLD-derived M maps for subsequent processing of OEF and CMRO2.
Figure 3 displays 3D images of T1-weighted magnitude, and baseline OEF and
CMRO2 maps, obtained via the dual-gas cBOLD and constrained qBOLD techniques.
OEF maps in qBOLD present a largely invariable contrast across the brain as is
expected from known physiology, whereas those in dual-gas cBOLD exhibit
regional variations. Nevertheless, statistical comparisons for GM-averaged
values via Bland-Altman plots (Figure 4) and paired t-tests suggest that both
OEF (p=0.07) and CMRO2 (p=0.71) measurements are not different between the two
methods.Discussion and Conclusions
We have performed
cross-validation of the constrained qBOLD technique with dual-gas cBOLD. Results
suggest that the two methods yield statistically insignificant differences in
OEF and CMRO2 quantifications for GM regions. Considering the need for a
specialized gas-breathing equipment in cBOLD, the present qBOLD method may be a
cost-efficient and patient-friendly alternative for assessment of cerebral oxygen
metabolism across the entire brain. Acknowledgements
NIH grant P41-EB029460 and R21-EB031364, and NRF Korea
grant 2021R1F1A1045621References
1. Ogawa S, Lee T-M, Kay AR, Tank DW. Brain magnetic resonance imaging
with contrast dependent on blood oxygenation. PNAS 1990;87(24):9868-72.
2. Bandettini PA. Twenty years of functional MRI: the science
and the stories. NeuroImage. 2012;62(2):575-88.
3. Blockley NP, Griffeth VE, Simon AB, Buxton RB. A review of
calibrated blood oxygenation level‐dependent (BOLD) methods for the measurement
of task‐induced changes in brain oxygen metabolism. NMR in Biomedicine.
2013;26(8):987-1003.
4. Davis TL, Kwong KK, Weisskoff RM, Rosen BR. Calibrated
functional MRI: mapping the dynamics of oxidative metabolism. Proceedings of
the National Academy of Sciences. 1998;95(4):1834-9.
5. Chiarelli PA, Bulte DP, Wise R, et
al. A calibration method for quantitative BOLD fMRI based on hyperoxia. Neuroimage
2007; 37: 808–820.
6. Bulte DP, Kelly M, Germuska M, et al.
Quantitative measurement of cerebral physiology using respiratory-calibrated
MRI. Neuroimage 2012; 60: 582–591.
7. Wise RG, Harris AD, Stone AJ, et al.
Measurement of OEF and absolute CMRO2: MRI-based methods using interleaved and
combined hypercapnia and hyperoxia. Neuroimage 2013;
83: 135–147.
8. An HY, Lin WL. Quantitative measurements of
cerebral blood oxygen saturation using magnetic resonance imaging. J Cereb Blood
Flow Metab 2000; 20:1225-1236.
9. He X,
Yablonskiy DA. Quantitative BOLD: mapping of human cerebral deoxygenated blood
volume and oxygen extraction fraction: default state. Magn Reson Med.
2007;57:115-126.
10. Lee H,
Englund EK, Wehrli FW. Interleaved quantitative BOLD: Combining extravascular
R2’- and intravascular R2-measurements for estimation of deoxygenated blood
volume and hemoglobin oxygen saturation. NeuroImage. 2018;174:420-431.
11. Lee H, Wehrli
FW. Whole-brain 3D mapping of oxygen metabolism using constrained quantitative
BOLD. NeuroImage 2022;250:118952.
12. Englund EK,
Fernández-Seara MA, Rodríguez-Soto AE, Lee H, Rodgers ZB, Vidorreta M, et al.
Calibrated fMRI for dynamic mapping of CMRO2 responses using MR-based
measurements of whole-brain venous oxygen saturation. Journal of Cerebral Blood
Flow & Metabolism. 2020;40(7):1501-1506.
13. Lee H, Wehrli
FW. Alternating unbalanced SSFP for 3D R2’ mapping of the human brain. Magn
Reson Med. 2021;85:2391-2402.
14. Lee H, Wehrli
FW. Venous cerebral blood volume mapping in the whole brain using
venous-spin-labeled 3D turbo spin echo. Magn Reson Med. 2020;84:1991-2003.
15. Vidorreta,
M., Wang, Z., Rodríguez, I., Pastor, M.A., Detre, J.A., Fernández-Seara, M.A.,
2013. Comparison of 2D and 3D single-shot ASL perfusion fMRI sequences.
Neuroimage 66, 662-671.