Eulanca Y. Liu1,2, Jia Guo3, Aaron B. Simon4, Frank Haist5, David J. Dubowitz2,6, and Richard B. Buxton2,6
1Neurosciences Graduate Program, Medical Scientist Training Program, University of California, San Diego, La Jolla, CA, United States, 2Center for Functional MRI, University of California, San Diego, La Jolla, CA, United States, 3Radiology, Stanford University, Stanford, CA, United States, 4Radiation Medicine and Applied Sciences, University of California, San Diego, La Jolla, CA, United States, 5Psychiatry, Center for Human Development, University of California, San Diego, La Jolla, CA, United States, 6Radiology, University of California, San Diego, La Jolla, CA, United States
Synopsis
We tested noninvasive
methods to measure absolute oxygen metabolism (CMRO2) in both baseline and
activation states without the use of special gases: VSEAN to measure baseline
O2 extraction fraction (OEF), and FLAIR-GESSE to measure R2’
to estimate the scaling parameter M. Primary findings were: M derived from R2’
had less variation across subjects compared to hypercapnia-derived M; OEF
values were in good agreement with previous PET findings; and, variation of baseline CBF/CMRO2 coupling
across subjects does not follow activation coupling, suggesting different
mechanisms may be involved. These results support the potential of gas-free
methods for quantitative physiological measurements.
Introduction
While methods for measuring cerebral blood flow
(CBF) and blood-oxygen-level dependent signal (BOLD) are well established, the
cerebral metabolic rate of oxygen (CMRO2) may provide a better
measure of neural activity by reflecting the energy cost of that activity, and may
potentially provide information on the activity of specific neural populations1,2. Current quantitative fMRI methods based on
simultaneous CBF/BOLD measurements during inhalation of CO2 enriched
and O2 enriched gases make it possible to measure absolute CMRO2
in both baseline and activation states3,4. However, the need for special gas administration requires
complicated experimental setup that limits wider application of these tools to
other research and clinical settings. Our goal was to evaluate the combination of
two gas-free techniques to make absolute baseline and activation CMRO2
measurements for more widespread applications.Experimental Approach
Baseline CMRO2: The baseline CMRO2
measurement is done with Velocity-Selective Excitation and Arterial Nulling
(VSEAN)5, which isolates the
signal of local venous blood and measures its relaxation rate R2.
Because R2 depends primarily on the O2 saturation of
hemoglobin, this provides a measurement of the local O2 extraction
fraction (OEF), and together with a baseline CBF measurement with ASL yields a
measurement of baseline CMRO2.
Activation CMRO2: In the classic
calibrated-BOLD3 method to measure the
fractional change in CMRO2 with activation, the BOLD signal model
includes a scaling parameter M that
is calculated from a separate measurement of CBF and BOLD responses to a
hypercapnia challenge3. Here, we instead use
a measurement of R2’, which, like M, reflects the baseline deoxyhemoglobin
content of a voxel. We measured R2’ with a FLuid Attenuated
Inversion Recovery Gradient Echo Sampling of Spin Echo (FLAIR-GESSE)6 technique, which has
an extensive literature building on early work of Yablonskiy and Haacke7. In the ideal case we
expect M~TE·R2’,
but an empirical scaling factor c is
needed to convert R2’ to M in a way that includes all of the effects
on the BOLD signal that are difficult to model, such as intravascular signal
changes, volume changes, and diffusion effects around small vessels:
$$M_{{R_{2}}'} = TE \times {R_2} ' \times c$$
Experimental Methods
Seventeen subjects (8F/9M) were examined with a
dual-echo spiral PICORE QUIPSS II ASL acquisition8 (TR=2.5s, TE1/2=3/30ms, 7 5mm-slices, gap=1mm) to
simultaneously measure CBF and BOLD dynamics. Flickering-checkerboard visual
stimulus was administered (two blocks, 1-min ON/1-min OFF) while the subject
performed a 1-back task presented at the center of the checkerboard as an active
baseline throughout the functional run and during the hypercapnia run (5%CO2 in air)3. An activated ROI in visual cortex was
identified with a separate functional localizer experiment. VSEAN5 (126reps, one 10mm-slice aligned to center of
ASL prescription, TR=3s) and FLAIR-GESSE6 (two scans: TE=63ms/83ms for early/late spin
echo series; asymmetrical sampling of decay curves; CSF nulling for middle
slice, TR=3.5s, TI=1.16s) were both collected in the baseline state. The total
acquisition time for VSEAN and GESSE data was 14 minutes. Post-processing and
analysis were performed as previously reported5,6,9,10.Results and Discussion
Table 1
summarizes the physiological measurements in the visual cortex ROI for the 17
subjects. The conversion factor from R2’·TE to M was c=0.994, unexpectedly close to 1 for this data. Primary findings were:
- Calibration data: M derived from R2’
showed much less variance across subjects than M from the hypercapnia
experiment (Figure 1), suggesting that R2’ may be a more precise
measurement. Excluding the one high value of R2’ as an outlier (>3 std dev), MR2’
ranged from 0.067 to 0.14, while MCO2 ranged from 0.022 to 0.30.
- OEF data: OEF measurements from
VSEAN (Figure 2) demonstrate values in good agreement with PET literature11,12. There was no correlation of OEF
with baseline CBF.
- CBF/CMRO2 coupling: The
slope of absolute CBF and CMRO2 was distinctly different for
variations in the baseline values and variations in the activation values
(Figure 3). This suggests that variations in the baseline state are not simply
variations of the “activation level” at rest for different subjects, but instead
may be set by different physiological mechanisms.
Conclusions
These results demonstrate the potential for
making absolute CMRO2 measurements without requiring the subject to
breathe special gases. However, work is still needed to refine these methods
and establish their validity. Each method has its own challenges: for VSEAN,
low SNR of the isolated blood signal for some voxels, and for FLAIR-GESSE, excessive
field distortion near edges. Nevertheless, these results support the
feasibility of painting a more complete picture of brain physiology, in
absolute terms, during both baseline and activation states, with the potential
of providing a deeper probe of neural activity.Acknowledgements
E. Y. Liu would like to acknowledge and thank Kenny Jackson, Abel Martinez, and Jessica Ho for their help in data acquisition; David Shin and Kun Lu for their advice and expertise with various imaging sequences and analyses; Interfaces Graduate Training Program and the UCSD Medical Scientist Training Program for support and funding. Lastly, the
authors would like to acknowledge NIH grant support through NS036722 and NS085478. References
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