Synopsis
When modelling the BOLD
response it is often assumed that arterial blood is fully oxygenated, and that
therefore contrast is driven solely by changes in venous oxygen saturation.
Recent evidence has emerged from rodent studies indicating that precapillary
arterioles may have an oxygenation level as low as 78%. Here, we assess
arterial oxygenation in vivo in humans by using short inversion time ASL in
normoxia, as well as hyperoxia. Our results suggest that imaging the BOLD
response may not be affected by partially oxygenated arterioles. Introduction
When modelling the blood
oxygenation level dependent (BOLD) response in the brain it is often assumed
that arterial haemoglobin (Hb) is fully oxygenated, and that therefore the
change in BOLD signal during functional hyperaemia is driven by changes in
venous Hb saturation
1. However, recent work in mice has shown that Hb oxygen saturation (SaO
2)
in cerebral precapillary arterioles can be as low as 78%
2, which suggests that arterial Hb saturation may affect measurement of
the BOLD response. Here, we aimed to non-invasively measure SaO
2
along the cerebral arterial tree in humans, by assessing T
2* of
arterial blood with short inversion time (TI) arterial spin labelling (ASL) in
normoxia and mild hyperoxia.
Methods
5 healthy volunteers (2 F, 27.2 ± 1.6
years) underwent a MRI scan session (3 T, GE HDx, Milwaukee, USA). Single slice
PICORE ASL images were acquired: TI = 450ms, TR =
600ms, 4 echoes = 3, 26, 49, and 72ms, number of time points = 3200, slice
along the anterior-posterior cingulate line, resolution = 3x3x7 mm3,
FOV = 198 mm, label thickness = 50 mm (10 mm below the imaging plane). There were 8 different levels of fixed inspired O2 (FiO2)
ranging from 21% (normoxia) to 42% in 3% increments. Each level lasted 4
minutes and was created by mixing medical air and 100% O2. Automated
flow controllers driven by in-house Matlab (R2012b) scripts ensured a
randomized order. Gases were delivered via a face mask. To
determine baseline arterial blood volume (aBV), a multi-TI PICORE ASL scan was
acquired at normoxia. Parameters: imaging and labelling
planes identical to the above scan; 8 TIs (150ms to 850ms, spacing 100ms);
variable TR (minimized); TE = 3ms; 320 time points (20 tag-control pairs
per TI). End-tidal
partial pressures of O2 and CO2 (PETO2
and PETCO2) were monitored throughout the scan.
A running subtraction was
performed per echo to obtain 4x1600
subtraction (ΔM) images. A mono-exponential decay over TE was
fitted to obtain time series of T2* (in ms) per voxel. To obtain average T2*
per FiO2, the parameter maps of the last minute of each hyperoxia
level were averaged together, i.e. when PETO2 was stable.
Maps of arterial blood volume (aBV) were used to create masks of large (aBVLarge
= aBV > 5 %v), medium (aBVMedium: 2 %v
< aBV < 5 %v), and small arteries (aBVSmall: 0.5 %v
< aBV < 2%v) (see Fig 1, where the anterior cerebral artery is
disregarded because of field inhomogeneity above the sinus). The aBV maps were
created by voxelwise fitting of an arterial input function3 to the average tag-control subtraction images from the multi TI scan at
normoxia. Average T2* for each hyperoxia level was calculated for
aBVLarge, aBVMedium, and aBVSmall.
Repeated measures ANOVA (RM-ANOVA) was used to investigate the effect of Hyperoxia and Artery Size on
the fitted T2*.
Results
The RM-ANOVA of the fitted T
2*
showed no significant interaction between
Hyperoxia and
Artery Size (F(14,56) = 2.15, p = 0.056), but significant effects
of
Hyperoxia (F(7,28) = 6.32, p < .01)
and
Artery Size (F(2,28) = 10.6, p <
.01). The T
2* for aBV
Large was significantly smaller than
for aBV
Small (paired t-test, p < .01, see Fig 2). Separate
RM-ANOVA per
Artery Size showed that there was
no effect of
Hyperoxia on T
2* in
aBV
Large (F(7,28) = 2.12, p = 0.10), but T
2* decreased in
aBV
Medium (F(7,28) = 4.63, p < 0.02) and aBV
Small
(F(7,28) = 4.69, p < 0.01).
Discussion
Absolute in vivo quantification of SaO
2 by T
2* measurements is difficult, because not only O
2
content, but also field inhomogeneity and blood flow velocity affect relaxation
4. The
low T
2* values in aBV
Large may therefore be due to
intravoxel dephasing with higher blood flow velocities
4, rather
than indicating low SaO
2. The decrease in T
2* with
hyperoxia as seen in aBV
Small may be caused by increased
sensitivity to local susceptibility changes induced by O
2 dissolved
in the blood plasma. Note that an increase in T
2* in aBV
Small
would have been expected at low levels of FiO
2, should baseline SaO
2 in small arteries have been low. Moreover, assuming low blood velocity in aBV
Small,
the baseline T
2* at normoxia (52.3 ± 8.2 ms) suggests that SaO
2
in aBV
Small is high (96%
5),
rather than low (78%
2). This
is possibly explained by insufficient resolution to be sensitive to arteriolar
SaO
2, which is reported to be spatially heterogeneous
2. Given
that a similar resolution is often used in functional imaging, partially
oxygenated arterioles may not interfere with measurement of the BOLD response.
Acknowledgements
No acknowledgement found.References
1. Buxton RB. Front Neuroenergetics. 2010;2(June):8.
2. Sakadžic S
et al. Nat Commun. 2014;5:5734.
3. Chappell MA
et al. Magn Reson Med. 2010;63(5):1357–65.
4. Kodama T et
al. Eur J Radiol. 1997;26(1):83–91.
5. Zhao JM et
al. Magn Reson Med. 2007;58(3):592–7.