Summary
Energy production in the brain depends almost exclusively on oxidative metabolism. Neurons have small energy reserves and require a continuous supply of oxygen (O2). It is therefore not surprising that one of the hallmarks of normal brain function is the tight coupling between cerebral blood flow and neuronal activity. Since capillaries are embedded in the O2-consuming neuropil, we have here examined whether activity-dependent dips in O2 tension drive capillary hyperemia. In vivo analyses showed that transient dips in tissue O2 tension elicit capillary hyperemia. Ex vivo experiments revealed that red blood cells (RBCs) themselves act as O2 sensors that autonomously regulate their own deformability and thereby flow velocity through capillaries in response to physiological decreases in O2 tension. This observation has broad implications for understanding how local changes in blood flow are coupled to synaptic transmission.
eTOC Blurb
Wei et al. demonstrate a novel mechanism for cerebral capillary blood flow regulation. Erythrocytes can sense and respond to decreases in environmental oxygen tension by autonomously increasing their flow velocities through capillaries and providing a rapid rise in oxygen supply.
Introduction
Neurovascular coupling is a process in which synaptic activity is linked to local changes in cerebral blood flow (Iadecola and Nedergaard, 2007; Kleinfeld et al., 2011). The mechanisms by which neural activity triggers hyperemia have been extensively studied because neurovascular coupling forms the basis for functional brain imaging. In addition, defects in neurovascular coupling may contribute to cognitive decline in neurodegenerative diseases such as Alzheimer disease, as well as in hypertension and stroke (Girouard and Iadecola, 2006). Functional hyperemia can be mediated by a number of compounds, many of which are byproducts of neural activity, including adenosine, nitric oxide (NO), prostaglandin E2 (PGE2), potassium ions (K+), epoxyeicosatrienoic acids (EETs), and carbon dioxide (CO2) (Iadecola and Nedergaard, 2007). In addition, functional hyperemia is preceded by a transient decrease in tissue oxygenation (Devor et al., 2011; Lecoq et al., 2011; Parpaleix et al., 2013). Since recent work has documented that functional hyperemia is initiated in microvessels embedded in the oxygen-(O2) consuming neuropil, we asked whether the initial dip in tissue O2 tension drives brain capillary hyperemia.
Results
Functional Hyperemia Begins In Capillaries and Is Inhibited When Oxidative Phosphorylation Is Suppressed
To identify the brain region activated by hindlimb stimulation, the exposed cortex was first visualized using intrinsic optical signaling (IOS) followed by high speed two-photon line-scanning to assess red blood cell (RBC) velocities in arterioles and capillaries in the contralateral sensory cortex of lightly sedated mice (Fig. 1A) (Bekar et al., 2012; Takano et al., 2006). Only cortical arterioles and capillaries located in the cortical region that exhibited the largest activity-dependent increase in IOS were analyzed. A comparison of the onset time of stimulation-induced elevation in RBC velocity revealed that capillary RBC velocities (0.67 ± 0.15 s, n = 65, 25 mice) increased prior to RBC velocities of upstream arterioles (2.33 ± 0.22 s, n = 61, 25 mice) (Fig. 1B), which is consistent with conclusions drawn by a prior study on vascular diameters (Hall et al., 2014). Additional analysis of a subset of connected capillaries and arterioles confirmed that following hindlimb stimulation, the onset of RBC velocity increases in capillaries preceded that of upstream arterioles (Fig. S1A). In these experiments, cortical vascular trees were mapped prior to data collection and corresponding arterioles and capillaries were identified for line-scanning. We also collected line scans orthogonally across vessel widths of arterioles and capillaries. These data showed that arterioles dilated at 2.38 ± 0.37 s, whereas capillary dilation occurred at 2.46 ± 0.22 s after hindlimb stimulation (n = 53–283, 15–18 mice) (Fig. 1C). In agreement with a recent publication, a slight dilation of capillaries was noted, but this occurred concomitant with arteriole dilation and most likely reflected pressure-induced increases in blood flow and/or volume (Hill et al., 2015). Thus, activity-dependent increases in capillary RBC velocities occur prior to both dilations of and RBC velocity increases in upstream arterioles, indicating that capillary hyperemia occurs before arterial hyperemia.
Figure 1. PO2 Dips Are Necessary to Elicit Capillary Hyperemia, See also Figure S1.
A. Experimental setup for assessing functional hyperemia elicited by sensory stimulation. Arterial blood pressure was monitored through a femoral artery catheter while the other hindlimb was stimulated. Through a cranial window, intrinsic optical signaling (IOS) was used to identify the cortical region of functional hyperemia. LFP and O2 sensor microelectrodes were placed in close proximity (10–20 μm) to one another within the activated region. During hindlimb stimulation, blood vessels in the activated contralateral hindlimb cortex were imaged using two-photon laser scanning microscopy. B. Time-course plot of hindlimb stimulation-evoked RBC velocity changes in cortical arterioles (red) and capillaries (black). Inset: IOS imaging (shown as a pseudocolor image) was used to identify the location of the activated hindlimb cortex in all experiments. Scale bar, 300 μm. Evoked RBC velocity increases began in capillaries (0.67 ± 0.15 s) prior to arterioles (2.33 ± 0.22 s). n = 61–65, 25 mice. ***, p < 0.001, t-test; **, p < 0.01, Mann-Whitney test. Black arrow indicates start of stimulation, black bar indicates duration of stimulation. C. Time-course plot of diameter changes of cortical arterioles (red) and capillaries (black). Arterioles began to dilate at 2.38 ± 0.37 s and capillaries at 2.46 ± 0.22 s after hindlimb stimulation. n = 53–283, 15–18 mice. ns, p > 0.05, Mann-Whitney test. D. Topical treatment with cyanide (100 μM) did not alter LFP power within the duration of the experiments. n = 13, 5 mice. ns, p > 0.05, paired t-test. E. Activity-dependent PO2 dips were suppressed by cyanide (1.92 ± 0.20 mmHg PO2 dip without NaCN, 0.67 ± 0.26 mmHg PO2 dip with NaCN). n = 36–47, 4–21 mice. ***, p < 0.001, Mann-Whitney test. Onset of the evoked PO2 dip was unchanged by cyanide (0.29 ± 0.09 s without NaCN, 0.46 ± 0.17 s with NaCN). n = 36–47, 4–21 mice. ns, p > 0.05, Mann-Whitney test. F. Activity-dependent increases in capillary RBC velocity was nearly abolished by cyanide (19.66 ± 3.83% without NaCN, 4.29 ± 1.20% with NaCN). n = 29–38, 6–13 mice. ***, p < 0.001, t-test. G. Activity-dependent penetrating arteriole vasodilation was unaffected by cyanide (4.95 ± 0.61% without NaCN, 4.79 ± 0.61% with NaCN). n = 66–79, 13–17 mice. ns, p > 0.05, Mann-Whitney test. H. Activity-dependent increases in cortical arteriole RBC velocity persisted in the presence of cyanide (8.22 ± 1.47% without NaCN, 8.36 ± 1.85% with NaCN). n = 35–43, 18–19 mice. ns, p > 0.05, Mann-Whitney test. Data are represented as mean ± SEM.
An intraparenchymal dip in partial pressure of oxygen (PO2) (Yacoub et al., 2001) began at 0.29 ± 0.09 s after hindlimb stimulation (Fig. 1E), similar to previous reports (Lecoq et al., 2011; Parpaleix et al., 2013), and thereby preceded capillary hyperemia by as much as 0.38 seconds. Could the transient dip in tissue PO2 be responsible for the initial phase of capillary hyperemia? To test this question, we applied sodium cyanide (NaCN), a potent inhibitor of cytochrome c oxidase and thus O2 utilization, to the exposed cerebral cortex. Initial experiments showed that 0.1 mM NaCN was the highest concentration that did not interfere with excitatory potentials evoked by hindlimb stimulation (Fig. 1D). Applying 0.1 mM NaCN on the pial surface increased resting PO2 (18.62 ± 2.51 mmHg PO2 before NaCN, 38.74 ± 4.40 mmHg PO2 after NaCN, n = 10 mice, p < 0.0001, paired t-test). NaCN also significantly suppressed stimulation-induced dips in tissue PO2 though it did not change the onset of the evoked PO2 dip (Fig. 1E). NaCN reduced the amplitude of capillary hyperemia by 78% (n = 29–38, 6–13 mice, p < 0.001, t-test) (Fig. 1F), but it did not attenuate activity-evoked penetrating arteriole vasodilation or velocity increases (Fig. 1G–H). This observation is surprising because the release of traditional smooth muscle relaxing mediators of functional hyperemia, including adenosine and K+, is potentiated rather than inhibited when oxidative phosphorylation is suppressed (Daval et al., 1980). The fact that NaCN application significantly suppressed capillary hyperemia alone is consistent with the idea that the activity-induced transient dip in tissue PO2 triggers an increase in local capillary RBC velocity.
PO2 Dips Are Sufficient to Elicit Capillary Hyperemia
We next asked whether a change in tissue PO2, in the absence of sensory activation, is sufficient to trigger capillary hyperemia. To address this question, three structurally different O2 scavengers, sodium ascorbate, sodium sulfite, or sodium dithionite, were separately microinjected near capillaries in the hindlimb cortex under the guidance of two-photon imaging (Fig. 2A). Ascorbate, sulfite, and dithionite all triggered a rapid decrease in local tissue PO2. Similar to activity-dependent responses, tissue PO2 exhibited a bi-phasic pattern, with an initial transient dip followed by a delayed and long-lasting overshoot (Fig. 2A). Strikingly, RBC velocity increased in nearby capillaries after microinjection of O2 scavengers, suggesting that tissue oxygenation influences capillary blood flow (Fig. 2B). For more detailed analyses, we focused on sulfite, which is converted to the relatively non-toxic compound, sulfate, after reaction with O2. We found that increasing the concentration of sulfite triggered a dose-dependent increase in RBC velocity (Fig. 2C). Sulfite microinjection also caused vasodilation of nearby penetrating arterioles, but the arteriolar vasodilation was delayed relative to sulfite-induced capillary velocity increases (Fig. 2D). Microinjection of the maximal concentration of sulfite (1 M) was not associated with detectable changes in the power spectrum of local field potential (LFP) activity (Fig. 2E). Thus, local application of O2 scavengers alone in the absence of sensory stimulation triggered hyperemia that closely resembled activity-dependent hyperemia. Moreover, sulfite elicited capillary hyperemia in both capillaries with and without pericytes in NG2-DsRed mice, suggesting that increases in RBC velocity occurred independent of pericyte presence (Fig. 2F). We defined capillaries with pericytes as capillaries in contact with pericyte cell bodies, and capillaries without pericytes as capillaries lacking contact with pericyte cell bodies. Next, we asked whether it is the depletion of O2 that directly triggers hyperemia, or whether hyperemia is induced indirectly by release of vasoactive mediators. To systematically address this we tested whether sulfite-elicited capillary hyperemia was reduced by pretreatment with inhibitors of NO production (L-NAME), inhibitors of PGE2 production (indomethacin), adenosine A1 and A2a receptor antagonists (DPCPX and SCH 58261), or inhibitors of inward rectifying K+ channels (barium). Topical application of these inhibitors to the pial surface all failed to suppress sulfite-induced capillary hyperemia (Fig. 2G), indicating that PO2-induced capillary hyperemia is not dependent on vascular smooth muscle relaxation.
Figure 2. PO2 Dips Are Sufficient to Elicit Capillary Hyperemia, See also Figure S2.
A. Left: Experimental setup used to study the effect of local application of O2 scavengers (sodium ascorbate, sulfite, or dithionite, 1 M). The O2 scavengers were delivered by a micropipette inserted 100–150 μm below the pial surface and placed < 50 μm from a capillary. Upon microinjection, O2 molecules within the vicinity of the pipette tip were trapped by the scavenger resulting in a transient drop in local O2 tension. Right: Local tissue PO2 was measured by an O2 sensor placed < 50 μm from the scavenger pipette tip and displayed a transient reduction in O2 tension followed by a PO2 overshoot. Black arrow indicates time of microinjection. B. Nearby capillary RBC velocity increased robustly after microinjection of any of the O2 scavengers: ascorbate, sulfite, or dithionite. Inset: A summary histogram of capillary RBC velocity changes induced by the transient reduction in tissue O2 tension. n = 23–34, 6–12 mice. **, p < 0.01, ***, p < 0.001, Kruskal-Wallis with Dunn’s test. C. Increasing the concentration of sulfite microinjected in close proximity to a capillary increased RBC velocity in a dose-dependent manner. n = 34–91, 4–12 mice. **, p < 0.01, ***, p < 0.001, Kruskal-Wallis with Dunn’s test. D. Sulfite microinjection (1 M) near penetrating arterioles resulted in arteriole vasodilation that was delayed relative to capillary velocity increases. n = 19–34, 5–12 mice. *, p < 0.05, t-test. E. Sulfite microinjection (1 M) did not alter neuronal activity (LFPs) detected at a distance of < 50 μm from the sulfite pipette tip. n = 21, 4 mice. ns, p > 0.05, paired t-test. F. Local sulfite microinjection increased RBC velocity in both capillaries with pericytes and without pericytes identified in NG2-DsRed reporter mice. n = 5–8, 6 mice. ns, p > 0.05, t-test. Purple bar indicates sulfite microinjection groups. G. Left: Inhibitors were topically applied to the cranial window prior to microinjection of sulfite. Right: A summary histogram of capillary RBC velocity changes induced by sulfite microinjection in the presence of the nitric oxide synthase (NOS) inhibitor L-NAME (2 mM), cyclooxygenase (COX) inhibitor indomethacin (500 μM), adenosine receptor inhibitors DPCPX and SCH 58261 (each 1 μM), K+ channel inhibitor barium (100 μM), and cytochrome c oxidase inhibitor cyanide (100 μM). n = 27–47, 5–6 mice. **, p < 0.01, ***, p < 0.001, compared to saline, Kruskal-Wallis with Dunn’s test. Data are represented as mean ± SEM.
To evaluate the contribution of pericytes to capillary hyperemia, we compared the amplitude and onset time of activity-induced RBC velocity increases of capillaries in contact with pericyte cell bodies with capillaries lacking contact with pericyte cell bodies in NG2-DsRed reporter mice. The baseline capillary diameter adjacent to the cell bodies of NG2-DsRed pericytes did not differ from segments of capillaries not in contact with pericyte cell bodies (Fig. S2A). We found that activity-evoked capillary hyperemia was unaffected by the presence or absence of an adjacent pericyte cell body. Capillary RBC velocity began at 0.71 ± 0.35 s in capillaries with pericytes (n = 28, 5 mice) and at 0.66 ± 0.22 s in capillaries without pericytes (n = 31, 5 mice) (Fig. S2B). Next, we evaluated pericyte expression of actin in mouse cortex using phalloidin staining of F-actin as well as α-smooth muscle actin (α-SMA) immunolabeling in fixed sections. Similar to prior studies, we defined the penetrating vessel as the zeroth branch order vessel, with subsequent branches labeled using increasing branch order numbers (Hall et al., 2014; Hill et al., 2015; Kornfield and Newman, 2014). Quantification confirmed that vessels beyond the third branch order were largely phalloidin and α-SMA negative (only 1.4% of vessels fourth order or higher, averaging 4.0 μm in diameter, were phalloidin and/or α-SMA positive, n = 49 vessels from 9 mice). In contrast, vessel branches zero to three were largely phalloidin and/or α-SMA positive (22–100% actin-positive, ranging from 5.4 to 13.3 μm in diameter, n = 12–25 vessels from 9 mice) (Fig. S2C). Only ~30% of DsRed+ pericyte cell bodies along branches one to three were actin-positive (Fig. S2D–E). These observations are in agreement with a recent study showing that smooth muscle actin is expressed by arterioles but not capillary mural cells in mouse and human neocortex (Hill et al., 2015). Hill et al. also showed that unlike smooth muscle actin-positive arterioles, pericyte-covered capillaries do not constrict or dilate in response to stimulation.
An important detail for validation of our in vivo analysis was our finding that 100% of DsRed-positive cells were PDGFRβ-positive and conversely that 100% of PDGFRβ-positive cells were DsRed-positive in NG2-DsRed reporter mice (Fig. S2F). In addition, DsRed-positive perivascular cells in NG2-DsRed reporter mice stained positively for desmin and CD13 in immunohistochemical slices (Fig. S2G). Therefore, capillaries identified as with or without pericytes during in vivo imaging of NG2-DsRed reporter mice were properly categorized, as PDGFRβ, desmin, and CD13 are pericyte-specific markers (Armulik et al., 2011).
AMPA Receptor Activity Modulates Capillary RBC Velocity
The velocity by which RBCs pass through capillaries is highly variable (Chaigneau et al., 2003; Kleinfeld et al., 1998; Stefanovic et al., 2008). Based on the observation of a tight coupling between postsynaptic AMPA receptor activity and tissue PO2 (Enager et al., 2009; Mathiesen et al., 2011), as well as our observation that NaCN inhibits both evoked PO2 dips and capillary hyperemia (Fig. 1E–F) while microinjection of O2 scavengers induces capillary hyperemia (Fig. 2B), we asked whether the ever-changing pattern of synaptic activity contributes to spontaneous fluctuations in capillary RBC velocity.
The AMPA receptor antagonist, CNQX (200 μM) was topically applied to the cerebral cortex and its effect on baseline (unstimulated) LFPs, PO2, and capillary RBC velocity was assessed. As a measure of baseline variability, we compared the standard deviation of LFPs, PO2, and capillary RBC velocity before and after application of CNQX (Fig. 3A–C). As expected, CNQX potently suppressed both the power and the standard deviation (SD) of baseline LFPs (Fig. 3A). Baseline PO2 levels also exhibited a significant increase (52.6% increase) and the variability of baseline PO2 was reduced (45.0% suppression of SD by CNQX) (Fig. 3B). Baseline capillary RBC velocity decreased by 25.7% and interestingly, the SD of RBC velocity fluctuations also fell significantly in response to CNQX (26.7% suppression by CNQX) (Fig. 3C), suggesting that AMPA-receptor mediated PO2 dips in part contribute to the variability of capillary RBC velocity at rest. Prior analyses have shown that cardiac- and respiration-dependent pulsatile blood flow is also in part responsible for the high variability in baseline capillary RBC velocities (Santisakultarm et al., 2012). Of note, baseline arterial diameter remained unchanged after addition of CNQX (Fig. 3D). To extend the analysis to include capillary functional hyperemia, we next compared responses to hindlimb stimulation before and after addition of CNQX. As expected, CNQX produced a dramatic decrease in excitatory potentials and PO2 dip amplitudes evoked by a 2-second hindlimb stimulation (81.0% and 90.1% suppression by CNQX, respectively) (Fig. 3E–F). Consistent with the key role of AMPA receptor activation in functional hyperemia, CNQX significantly delayed the onset and suppressed the amplitude of capillary RBC velocity increases in response to hindlimb stimulation (75.0% suppression by CNQX) (Fig. 3G). Figures 3H–I compare the relative power by which blockade of AMPA receptors suppressed spontaneous fluctuations and stimulation-dependent changes in LFPs, PO2, and capillary RBC velocity. Of note, inhibition of NMDA receptors (AP5, 500 μM) did not have a significant effect on capillary hyperemia (Fig. S3). This observation is consistent with the idea that excitatory transmission is primarily the result of AMPA receptor activation in the sensory cortex (Hoffmeyer et al., 2007; Self et al., 2012).
Figure 3. Capillary RBC Velocity Is Modulated by AMPA Receptor Activity, See also Figure S3.
The AMPA receptor inhibitor CNQX (200 μM) was added to the aCSF covering the cranial window for 30–45 minutes and recordings with and without CNQX were compared. A. Comparison of spontaneous (unstimulated) LFP activity (power at 4–32 Hz), as well as standard deviation of spontaneous LFP activity before and after CNQX. n = 6 mice. *, p < 0.05, **, p < 0.01, t-test. B. Comparison of baseline PO2 level and the spontaneous variability (standard deviation) of PO2 before (21.65 ± 3.77 mmHg baseline and 1.09 ± 0.24 mmHg SD) and after (33.03 ± 2.64 mmHg baseline and 0.60 ± 0.11 mmHg SD) CNQX. n = 6–8 mice. **, p < 0.01, *, p < 0.05, paired t-test. C. Comparison of baseline capillary RBC velocity and the spontaneous variability of RBC velocity before (0.70 ± 0.04 mm/s baseline and 0.15 ± 0.007 mm/s SD) and after (0.52 ± 0.03 mm/s baseline and 0.11 ± 0.006 mm/s SD) CNQX. n = 131–191, 12–13 mice. **, p < 0.01, ***, p < 0.001, Mann-Whitney test. D. CNQX did not alter the baseline diameters of penetrating arterioles (16.71 ± 1.48 μm before CNQX, 17.35 ± 1.28 μm after CNQX). n = 30, 7 mice. ns, p > 0.05, Wilcoxon test. E. Comparison of excitatory potentials evoked by hindlimb stimulation quantified as the LFP power at 10 Hz before and after CNQX. n = 15–23, 3–4 mice. **, p < 0.01, t-test. Black arrow indicates start of stimulation. F. Hindlimb stimulation-induced PO2 dips were suppressed by CNQX (1.92 ± 0.20 mmHg in controls, 0.19 ± 0.10 mmHg after CNQX). n = 29–47, 9–21 mice. ***, p < 0.001, Mann-Whitney test. G. Activity-dependent increases in capillary RBC velocity were reduced by CNQX. Bar histograms compare activity-induced capillary RBC velocity increases and onset times without (16.76 ± 2.76% increase and 0.73 ± 0.23 s onset) and with (4.19 ± 1.68% increase and 2.41 ± 0.56 s onset) CNQX. n = 49–54, 10–13 mice. ***, p < 0.001, *, p < 0.05, Mann-Whitney test. Black arrow indicates start of stimulation, black bar indicates duration of stimulation. H. Suppression of spontaneous variability in LFPs, PO2, and capillary RBC velocity before and after CNQX as measured by standard deviation. I. Suppression of activity-induced changes in LFPs, PO2 dip, and capillary RBC velocity by CNQX. Data are represented as mean ± SEM.
Together, these results suggest that O2-consuming synaptic activity is partly responsible for the variability of cortical capillary RBC velocities during resting conditions, and primarily responsible for the initiation of activity-dependent capillary hyperemia.
Oxygen Depletion Alone Is Sufficient to Increase RBC Velocity ex vivo
The observation that microinjection of O2 scavengers induced pericyte- and vasoactive mediator-independent capillary hyperemia led us to hypothesize that O2 tension itself, independent of the neurovascular unit, can control RBC deformation and thus RBC flow through capillaries. To test this idea in the absence of the neurovascular unit, we turned to an ex vivo assessment of the effect of oxygenation on RBC flow through an artificial capillary. We employed a microfluidic device in which isolated human RBCs pass through a narrow flow channel (Fig. 4A) (Abkarian et al., 2006; Cinar et al., 2015; Wan et al., 2011; Wan et al., 2008). This approach allowed an evaluation of RBC velocity in the absence of the cellular components of the neurovascular unit, i.e. endothelial cells, pericytes, and astrocytes (Petzold and Murthy, 2011). Since the capillary lumen is considerably smaller than RBC diameters, RBC deformability is a major determinant of the speed by which the RBC passes through a capillary (Chaigneau et al., 2003). A microfluidic device made of polydimethylsiloxane (PDMS) was submerged in a chamber containing sodium sulfite, an O2 scavenger. Since PDMS is O2, but not H2O permeable, the chamber functioned as a sink for O2 (Fig. 4A). A colorimetric calibration, based on adding the O2-sensing dye, tris(2,2′-bipyridyl)dichlororuthenium(II) hexahydrate, to deionized (DI) water showed that PO2 in the flow channel was an inverse function of the sulfite concentration (0 to 2 M) (Fig. 4B). Remarkably, the velocity of RBCs flowing through the channel increased as a function of O2 depletion, indicating that brief deoxygenation alone can affect the mechanical properties of RBCs (Fig. 4B–C). The O2-dependent increase in RBC velocity was observed when RBCs were resuspended in either plasma or PBS (Fig. 4C). Because PO2 in capillaries is highly variable and can range from ~5–95 mmHg but tends to be on the lower end of that range within true microvessels (Kasischke et al., 2011; Parpaleix et al., 2013; Sakadzic et al., 2014), we focused on the effects of relatively lower PO2. In these experiments, the PBS was first purged with N2 until the PO2 reached 34 mmHg, approximating normal brain PO2 (Jaeger et al., 2005). Similar to above, RBCs were driven through a microfluidic chamber immersed in a sulfite sink (0 to 1 M) and colorimetrically calibrated (Fig. 4B). This analysis showed that at a relatively lower range of O2 tension, RBC velocities became more sensitive to surrounding changes in PO2 (p < 0.001, t-test with Bonferroni test, compared to PBS without N2 purging and plasma) (Fig. 4C–D). Interestingly however, increasing the O2 from 21% to 100% (or from PO2 ~160 mmHg to ~760 mmHg) failed to alter RBC velocity in the microfluidic capillary (1.000 normalized velocity in 21% vs 0.998 normalized velocity in 100% O2, n = 9–19, p > 0.05, t-test), consistent with the notion that at superphysiologic PO2, hemoglobin continues to be maximally saturated with O2 and RBCs reach the limit of their ability to bind additional O2 and respond with velocity changes. Classical studies have shown that in response to deoxygenation and/or mechanical stress, RBCs release ATP which activates endothelial cell purinergic receptors (P2YR1s) resulting in NO release. In turn, NO or other endothelium-dependent vasodilators increase blood flow in hypoxic tissues via arterial smooth muscle relaxation (Chen et al., 2014; Ellsworth et al., 2009; Jia et al., 1996). RBCs may also directly release NO from S-nitroso-Hb upon deoxygenation (Jensen, 2009). However, we found that the PO2-elicited increase in RBC flow velocity was not a result of direct ATP or NO release. Exposing RBCs to the ATP-degrading enzyme apyrase (40 U/mL) or the NO synthase inhibitor L-NAME (3 mM) did not affect PO2-induced elevations in RBC velocity (Fig. 4D), in accordance with the in vivo observation that L-NAME failed to suppress capillary hyperemia (Fig. 2G). In addition, CNQX had no effect on PO2-induced increases in RBC velocity through the microfluidic channel (Fig. 4D). When RBCs were treated with K+ channel inhibitors (4-aminopyridine (4-AP, non-selective voltage-dependent K+ channel blocker, 1 mM), charybdotoxin (Ca2+-activated voltage-gated K+ channel blocker, 100 nM), or iberiotoxin (large-conductance Ca2+-activated K+ channel blocker, 100 nM)), however, the sensitivity of RBC velocity to PO2 changes decreased (Fig. 4E), suggesting that K+ flux across the membrane plays a role in the velocity of RBC flow in capillaries. As a negative control, RBCs were treated with diamide, which stiffens the RBC membrane by crosslinking the cytoskeletal spectrin network (Fischer et al., 1978; Wan et al., 2008). The flow velocity of diamide-exposed RBCs was unaffected by PO2, supporting the notion that the PO2-induced increase in RBC flow velocity is due to increased deformability of the RBC membrane (Fig. 4D).
Figure 4. Oxygen Depletion Alone Is Sufficient to Increase RBC Velocity ex vivo.
A. A diagram of the experimental setup for ex vivo analysis of the effect of PO2 on RBC flow velocity. Human RBCs (~7 μm in diameter) were added to the bath containing PBS and forced to flow through a microfluidic device containing a narrow channel (5 μm) by applying a constant pressure (1.6 psi). The microfluidic device was submerged in an O2 sink (chamber containing H2O with 0.0, 0.01, 0.1, or 1.0 M sodium sulfite). PO2 in the microfluidic channel was successively lowered by increasing the concentration of sulfite in the O2 sink (0.0–1.0 M). RBC motion was captured by a high-speed camera. w: width. B. Left: To colorimetrically quantify PO2 in the capillary channel, 25 μM of tris(2,2′-bipyridyl)dichlororuthenium(II) hexahydrate was prepared in N2-bubbled deionized (DI) water (n = 3) and in air-saturated DI water (n = 4). The change in fluorescence intensity of the O2 indicator dye solution flowing through the microfluidic device was measured during exposure to 0.0, 0.01, 0.1, 1.0, 1.5 and 2.0 M sodium sulfite solution and converted to PO2. Right: Images comparing RBC flow within an O2 sink containing 0 or 1 M sulfite. Images of flowing RBCs captured by the high-speed camera at sequential time points are superimposed. T: time. C. Lowering PO2 in the microfluidic channel caused an increase in RBC velocity. Responsiveness of RBCs to surrounding PO2 levels did not differ regardless of resuspension in PBS (n = 214, RBC velocity (mm/s) = −0.137 × PO2 (mmHg) + 80.056, R2 = 0.910) or plasma (n = 42, RBC velocity (mm/s) = −0.157 × PO2 (mmHg) + 69.069, R2 = 0.995). p > 0.05, t-test with Bonferroni test. D. The starting PO2 in the PBS bath was lowered to 34 mmHg by N2 purging prior to immersion in the O2 sink, and RBC velocity continued to be sensitive to surrounding PO2 changes (n = 71, RBC velocity (mm/s) = −0.451 × PO2 (mmHg) + 82.074, R2 = 0.999). Dephosphorylation of extracellular ATP by apyrase (40 U/ml) or inhibition of NOS and AMPA receptors by L-NAME (3 mM) and CNQX (200 μM), respectively, did not alter RBC velocity increases in response to lowering surrounding PO2. n = 5–74. p > 0.05, one-way ANOVA. When diamide (200 μM) was added to stiffen RBC membranes, lowering PO2 failed to increase RBC velocity compared to controls. n = 70–71. p < 0.0001, t-test. E. In the presence of the potassium channel inhibitors 4-aminopyridine (4-AP) (1 mM) (n = 199, RBC velocity (mm/s) = −0.299 × PO2 (mmHg) + 82.304, R2 = 0.992), charybdotoxin (100 nM) (n = 197, RBC velocity (mm/s) = −0.278 × PO2 (mmHg) + 82.277, R2 = 0.993), or iberiotoxin (100 nM) (n = 188, RBC velocity (mm/s) = −0.213 × PO2 (mmHg) + 78.011, R2 = 0.944), the sensitivity of RBC velocity to the change in PO2 was reduced. n = 188–199. p < 0.05, one-way ANOVA. F. A schematic of the experimental setup for ex vivo analysis of the effect of PO2 on RBC deformability. RBCs suspended in a N2-purged PBS solution were injected into a microfluidic device containing a constriction (width = 20 μm) and constant pressure (1.6 psi) was applied. The microfluidic device was submerged in an O2 sink similar to Fig. 4A, and RBC motion was captured by a high-speed camera. The deformability of RBCs was characterized by the elongation index DL/DW, where DL and DW represent the length and thickness of a RBC flowing through the constriction. G. The elongation index (DL/DW) of RBCs increased with a decrease in surrounding O2 levels for control RBCs (n = 239, RBC DL/DW = −0.0237 × PO2 (mmHg) + 4.0886, R2 = 0.993). Compared to control RBCs flowing through the channel, diamide-treated (200 μM) RBCs did not deform significantly in response to changes in PO2. n = 88–239. p < 0.0001, t-test. H. Elongation indexes (DL/DW) of control RBCs and RBCs treated with 4-AP (1 mM) (n = 276, RBC DL/DW = −0.0373 × PO2 (mmHg) + 4.0224, R2 = 0.997), charybdotoxin (100 nM) (n = 256, RBC DL/DW = −0.0386 × PO2 (mmHg) + 4.0795, R2 = 0.992), or iberiotoxin (100 nM) (n = 208, RBC DL/DW = −0.0377 × PO2 (mmHg) + 4.0085, R2 = 0.992) at different O2 tensions are shown. n = 208–276. p < 0.05, one-way ANOVA.
To directly test whether RBC deformability is controlled by PO2, we assessed the shear-induced deformability of RBCs flowing in a relatively large-sized microfluidic channel containing a segment of constriction (width = 20 μm) (Fig. 4F). The shear-induced deformability of RBCs was characterized by the elongation index DL/DW where DL and DW represented the length and thickness of a RBC flowing through the constriction, respectively (adapted from (Forsyth et al., 2010; Mohandas et al., 1980)). We found that the elongation of RBCs in response to shear stress increased as PO2 decreased, demonstrating that RBCs are more flexible in lower PO2 conditions (Fig. 4G). The dependence of RBC deformability on PO2 was significantly diminished when diamide was added (Fig. 4G). RBCs treated with the K+ channel blockers 4-AP (1 mM), charybdotoxin (100 nM), or iberiotoxin (100 nM) also exhibited reduced sensitivity to PO2 changes compared to controls (Fig. 4H). These data show that lowering PO2 increases RBC deformability and thereby the velocity by which RBCs pass through a narrow ex vivo capillary lacking endothelial cells, pericytes, and astrocytes. Exposure to K+ channel inhibitors reduced the deformability of RBCs and thus the potency by which PO2 increased RBC flow velocity. This latter observation is consistent with prior studies documenting that a decrease in cell volume mediated by K+ efflux and water loss may play a role in permitting RBC deformation during the shear stress associated with squeezing through a narrow capillary (Cinar et al., 2015).
Exchanging RBCs For An O2-Carrying Blood Substitute Suppresses Functional Hyperemia in vivo
Our ex vivo data suggest that RBCs autonomously regulate their own velocities through capillaries in response to changes in surrounding PO2 tension. If this finding is relevant in vivo, we would expect that in vivo capillary hyperemia is suppressed when RBCs are replaced by an acellular hemoglobin-based O2 carrier (HBOC). To meticulously test whether RBCs are required for activity-dependent capillary hyperemia, we partially exchanged the blood in our mouse model with a synthetic HBOC, i.e. polymerized hemoglobin (PolyHb) (Baek et al., 2012; Zhou et al., 2011). We were able to decrease the hematocrit by 80.3 ± 0.5% (10.55 ± 0.11 vs. 2.08 ± 0.046 106 cells per μL) by gradually replacing RBCs with PolyHb. Mixing PolyHb with whole blood did not alter blood viscosity (Fig. 5A). PolyHb blood exchange did not alter resting cortical PO2, sensory-induced dips in PO2 (Fig. 5B), or sensory-evoked electrical activity (evoked LFP 10 Hz power was 0.017 ± 0.0085 mV2 in control mice and 0.015 ± 0.0064 mV2 in PolyHb mice, p > 0.05, t-test). It did, however, delay the onset time and reduce the amplitude of activity-dependent capillary hyperemia (Fig. 5C–D). Basal cortical arteriole diameters were unchanged but evoked arteriole vasodilation was reduced with PolyHb (Fig. 5E). With an insufficient RBC population, capillary hyperemia may be primarily driven by upstream arteriole vasodilation.
Figure 5. Oxygen Carriage by Erythrocytes Is Required for Functional Hyperemia.
A. Left: Capillary line-scan images from a control and PolyHb-exchanged mouse. Right: PolyHb blood exchange does not alter blood viscosity. B. Left: Baseline tissue PO2 is unchanged by PolyHb blood exchange (17.31 ± 2.62 mmHg in controls, 16.59 ± 4.27 in PolyHb). n = 7–14 mice. ns, p > 0.05, Mann-Whitney test. Right: PO2 dip in response to hindlimb stimulation is similar between mice with and without PolyHb blood exchange (1.92 ± 0.20 mmHg PO2 dip in controls, 1.76 ± 0.20 mmHg PO2 dip in PolyHb). n = 36–47, 6–21 mice. ns, p > 0.05, Mann-Whitney test. C. Capillary RBC velocity responses during hindlimb stimulation in mice with PolyHb blood replacement. Black arrow indicates start of stimulation, black bar indicates duration of stimulation. D. Left: Baseline capillary RBC velocity in mice with (0.59 ± 0.08 mm/s) and without (0.75 ± 0.06 mm/s) PolyHb blood exchange. n = 23–65, 8–25 mice. ns, p > 0.05, Mann-Whitney test. Right: Comparison of capillary RBC velocity increases in response to hindlimb stimulation (19.15 ± 2.57% in controls, 9.97 ± 4.15% in PolyHb). Onset time of capillary velocity changes (0.67 ± 0.15 s in controls, 2.02 ± 0.42 s in PolyHb). n = 23–65, 8–25 mice. *, p < 0.05, Mann-Whitney test, ***, p < 0.001, t-test. E. Left: Baseline arteriole diameter in mice with (17.14 ± 0.85 μm) and without (17.40 ± 0.68 μm) PolyHb blood exchange. n = 32–53, 6–18 mice. ns, p > 0.05, t-test. Right: % evoked arteriole vasodilation in mice with (2.30 ± 0.71%) and without (5.47 ± 0.99%) PolyHb blood exchange. n = 32–53, 6–18 mice. *, p < 0.05, Mann-Whitney test. F. Left: Inspired 100% O2 increases baseline brain parenchymal PO2 (26.80 ± 6.24 mmHg PO2 in room air, 52.89 ± 16.75 mmHg PO2 in 100% O2). n = 15 mice. ***, p < 0.001, Wilcoxon test. Right: Hindlimb stimulation-induced PO2 dips were preserved in mice ventilated with 100% O2 (1.92 ± 0.20 mmHg PO2 dip in room air, 1.86 ± 0.61 mmHg PO2 dip in 100% O2). n = 14–47, 10–21 mice. ns, p > 0.05, Mann-Whitney test. G. Left: Baseline capillary RBC velocity in mice ventilated with room air and 100% O2 (0.75 ± 0.06 mm/s in room air, 0.56 ± 0.05 mm/s in 100% O2). n = 32–65, 11–25 mice. *, p < 0.05, Mann-Whitney test. Right: Baseline cortical arteriole diameter in mice ventilated with room air and 100% O2 (24.96 ± 2.06 μm in room air, 24.94 ± 2.34 μm in 100% O2). n = 10, 3 mice. ns, p > 0.05, paired t-test. H. Left: Hindlimb stimulation-evoked capillary RBC velocity increases (19.15 ± 2.57% in room air, 13.44 ± 2.25% in 100% O2). n = 32–65, 11–25 mice. ns, p > 0.05, Mann-Whitney test. Right: Onset time of capillary RBC velocity changes (0.67 ± 0.15 s in room air, 0.79 ± 0.27 s in 100% O2). n = 32–65, 11–25 mice. ns, p > 0.05, Mann-Whitney test. Data are represented as mean ± SEM.
How does hyperoxygenation affect the microcirculation? Breathing 100% O2 elevated baseline cortical PO2 from ~25 to ~50 mmHg (Jaeger et al., 2005), without causing significant changes in the evoked PO2 dip (Fig. 5F). Basal capillary RBC velocities were reduced while basal arteriole diameters and capillary hyperemia were unchanged (Fig. 5G–H). Hence, both the ex vivo and in vivo observations provide strong support for the notion that deoxygenation-mediated changes in erythrocyte deformability drive capillary hyperemia.
Discussion
Despite the uncontested tight linkage between neural activity and vascular responses, the question of what drives functional hyperemia is still debated. In principle, a mechanism sensing depletion of an energy substrate (O2 or glucose) or alternatively the release of vasoactive mediators (NO, PGE2, ATP, adenosine, K+, and other molecules) could drive activity-dependent increases in blood flow. In this work, we took advantage of the discovery that functional hyperemia is initiated in microvessels rather than in arterioles (Hall et al., 2014). We confirmed that capillary RBC velocity increases 1–2 seconds prior to arterial hyperemia, but similar to a recent study (Hill et al., 2015) failed to identify pericytes as the principal regulator of capillary hyperemia. Several experimental findings presented here implicate the transient PO2 dip in the initiation of the activity-dependent increase in capillary perfusion via a mechanism independent of the release of vasoactive agents and smooth muscle relaxation, including: (1) Capillary functional hyperemia was suppressed when oxidative metabolism was inhibited by local application of NaCN. Not only does this observation support the notion that PO2 regulates capillary perfusion, but it also indirectly provides evidence against a central role of vasoactive mediators in initiating functional hyperemia, since adenosine, lactate, and K+ release are all increased when oxidative metabolism is inhibited (Daval et al., 1980). (2) The AMPA receptor blocker CNQX suppressed the spontaneous fluctuations in resting PO2 and capillary RBC velocity by 45.0% and 26.7%, respectively, indicating that AMPA receptor activity in part drives spontaneous changes in O2 tension and capillary RBC flow. Moreover, activity-induced PO2 dips (90.1%) and capillary hyperemia (75.0%) were both potently suppressed by CNQX. (3) Microinjection of O2 scavengers induced capillary hyperemia in the absence of an increase in neural activity. The hyperemia induced by local scavenging of O2 was not suppressed by antagonists of adenosine A1 and A2A receptors or inhibitors of K+ channels, NO and PGE2 production, or O2 consumption (NaCN). (4) Ex vivo quantification of the velocity of RBCs moving through a microfluidic channel under strict PO2 control showed that RBC velocity increased as a direct function of physiologically relevant decreases in PO2. Transient manipulation of PO2 within the range of 0–160 mmHg directly controlled not only the velocity by which RBCs traveled through a narrow synthetic channel in the absence of endothelial cells, pericytes, and astrocytes, but also RBC deformability in response to shear stress. In contrast, elevation of PO2 (100% O2) considerably past physiologic levels failed to decrease RBC velocity beyond what was observed in room air (~21% O2). (5) Partial replacement of intravascular RBCs with a synthetic RBC-free blood substitute in vivo showed that lowering the hematocrit by ~80% was associated with a significant reduction in activity-dependent capillary hyperemia. Together, these observations provide evidence to support the novel concept that RBCs are not only sensors of PO2 but can also regulate their deformability and thereby the velocity with which they pass through capillaries in response to transient drops in tissue oxygenation.
The effect of PO2 on RBC deformability is debated, possibly because most past studies were based on indirect measurements that have not been readily reproducible (Kim et al., 2015; Martindale and McKay, 1995; Yoon et al., 2009). To our knowledge no prior studies have directly quantified changes in RBC velocity and deformability in response to transient changes in PO2. The data presented here using an ex vivo microfluidic approach demonstrate a direct relationship between RBC velocity and deformability elicited by transient decreases in PO2.
Deoxygenation of RBCs leads to displacement of ankyrin from band 3, resulting in release of the spectrin/actin cytoskeleton from the cell membrane (Stefanovic et al., 2013). The weakening of membrane-cytoskeletal interactions has been proposed to be beneficial to blood flow during brief periods of deoxygenation (Stefanovic et al., 2013) and may contribute to increased RBC deformability during drops in PO2. Prior studies in peripheral tissues have shown that RBCs can induce hyperemia but pointed to a mechanism that involves ATP release from RBCs (under shear-induced deformation and/or hypoxia), which triggers endothelial cell NO production that subsequently dilates arteries by hyperpolarizing vascular smooth muscle cells (Ellsworth et al., 2009). Our microfluidic chamber experiments showing that lowering PO2 in the absence of the neurovascular unit increased isolated RBC velocity, coupled with the finding that L-NAME (an inhibitor of NO synthase) had no effect on capillary hyperemia, argue against a significant contribution from this paracellular signaling mechanism. Furthermore, PO2-induced arteriole dilation was delayed relative to PO2-induced capillary blood flow increases, mimicking hyperemia elicited by sensory input and signifying that arteriole vasodilation is not the primary driver of PO2-dependent capillary hyperemia. Previously, the existence of an O2-sensing mechanism has been questioned based on the finding that regional functional hyperemia persisted in hyperbaric hyperoxia (Lindauer et al., 2010). We here confirmed that capillary hyperemia was preserved in hyperoxia but extended the analysis to show that activity-induced PO2 dips persisted during hyperoxic conditions. Thus, hyperoxia did not suppress either activity-induced PO2 dips or capillary hyperemia. Additionally, inhibiting metabolic O2 consumption by application of cyanide blocked both activity-dependent dips in PO2 and capillary hyperemia irrespective of the baseline tissue PO2. Collectively, these sets of data suggest that it is the transient PO2 dip rather than baseline PO2 that triggers capillary hyperemia. This conclusion is further supported by our ex vivo observation that RBC velocity in the microfluidic device increased in response to PO2 reductions across a wide range of physiological PO2 levels (0–160 mmHg).
It is important to note that functional hyperemia outlasted the dip in PO2. Accordingly, only the very initial phase (< 1.5 s) of capillary hyperemia that precedes arterial dilation is driven by activity-induced dips in PO2. The initial capillary response during functional hyperemia may serve as the rapid phase of hyperemia that supplies active neurons with immediately available O2. The delayed and sustained hyperemic phase is most likely powered by the slower dilation of upstream arterioles and serves to prevent a prolonged drop in oxygenation at tissue located more remotely from arterioles and proximal capillaries (Devor et al., 2011; Leithner and Royl, 2014). It is unclear whether PO2-mediated rapid capillary hyperemia directly causes delayed arteriole vasodilation, as it has been shown that release of vasoactive agents from both interneurons and astrocytes can trigger arteriole dilation (Cauli and Hamel, 2010; Takano et al., 2006). Capillary hyperemia and arteriole hyperemia may have independent regulatory mechanisms that work in a concerted manner to optimize blood supply. Alternatively, the delayed dilation of upstream arterioles may be a consequence of PO2-induced rapid capillary hyperemia, mediated by the propagation of Ca2+ signals along the neurovascular unit (Fig. 6). If so, it is interesting to speculate whether the impaired vasoreactivity observed in various diseases and in aging is a consequence of impaired PO2-mediated capillary hyperemia. Future studies can address the relationship between capillary hyperemia and delayed arteriole dilation. Further experiments can also assess sensory-evoked capillary hyperemia in awake behaving mice.
Figure 6. Model of Capillary Hyperemia and Potential Link to Upstream Arteriole Dilation.
(1) Sensory input triggers local neural activation resulting in (2) a local dip in tissue and plasma O2 tension (Parpaleix et al., 2013). The dip in plasma O2 tension changes the mechanical properties of RBCs resulting in (3) an increase in RBC velocity. The transient dip in O2 tension drives the fast, initial phase of capillary hyperemia. The rise in RBC velocity in both capillaries and arterioles rapidly increases O2 delivery resulting in an O2 overshoot (4–5). The delayed and more sustained phase of capillary hyperemia is driven by vasodilation of upstream arterioles. It is not known whether the initial phase of capillary hyperemia, which is driven by a dip in local PO2, is mechanistically linked to the delayed dilation of the upstream arteriole. Hypothetical pathways of signal propagation along the neurovascular unit include Ca2+ signaling in endothelial cells, pericytes, or vascular endfeet of astrocytes. Also, it is possible that an initial increase in capillary perfusion results in pressure changes that trigger a myogenic response in the upstream arteriole. Finally, capillary hyperemia and arteriole vasodilation may be initiated independently. Several mechanisms, including release of vasoactive mediators from interneurons or astrocytes, are known to directly cause arteriole vasodilation (Cauli and Hamel, 2010; Iadecola and Nedergaard, 2007).
Functional hyperemia is an integrated response that tightly couples O2 consumption with O2 supply. Here we show that both spontaneous and activity-induced dips in tissue PO2 drive the earliest phase of capillary hyperemia. Furthermore, PO2 directly controls the velocity by which RBCs transit through a narrow channel in a microfluidic device. Thus, RBCs may themselves serve as autonomous regulators of capillary perfusion that operate independently of the neurovascular unit and the release of vasoactive molecules. The idea that erythrocytes – the major suppliers of O2 – function not only as O2 carriers but also as O2 sensors and regulators of capillary blood flow provides a simple, yet swift and precise mechanism for controlling the cerebral microcirculation.
Experimental Procedures
Animals
C57Bl6 mice (25–30 g, 8–12 weeks old, The Jackson Laboratory) and NG2-DsRed mice (Tg(Cspg4-DsRed.T1)1Akik/J, RRID: IMSR_JAX:008241) (Zhu et al., 2008) on a C57Bl6 background of either sex were utilized. Mice were prepared for in vivo imaging as described previously (Bekar et al., 2008; Ding et al., 2013; Wang et al., 2006; Xie et al., 2013) and in the Supplemental Experimental Procedures.
Physiological manipulations and measurements
Physiological manipulations and measurements were performed as previously described (Baek et al., 2012; Bekar et al., 2012; Kasischke et al., 2011; Takano et al., 2007; Vazquez et al., 2011; Xie et al., 2013; Zhou et al., 2011) and in the Supplemental Experimental Procedures.
Microfluidic device and RBC imaging
Microfluidic device construction and human RBC imaging were performed as previously described (Duffy et al., 1998; Wan et al., 2011; Wan et al., 2008) and in the Supplemental Experimental Procedures.
Intrinsic optical signal and two-photon imaging
Intrinsic optical signaling (IOS), two-photon imaging, and immunofluorescence imaging were performed as previously described (Armulik et al., 2011; Bekar et al., 2012) and in the Supplemental Experimental Procedures.
Statistics
All data were expressed as mean ± SEM. Normality of the data was evaluated with the Shapiro-Wilk test, and non-parametric tests were used when normality was not assumed. A Student’s t-test or Mann-Whitney test was used to compare two groups. A one-way ANOVA with a Bonferroni’s multiple comparison test or a Kruskal-Wallis test with a Dunn’s multiple comparison test was used to compare multiple groups. A paired t-test or Wilcoxon matched-pairs signed rank test was used for pairwise comparisons. p < 0.05 was considered significant.
Supplementary Material
Highlights.
Activity-dependent cortical hyperemia begins in capillaries
Transient dips in tissue O2 tension drive capillary hyperemia
Depletion of O2 increases isolated erythrocyte flow velocity ex vivo
Erythrocytes are O2 sensors that regulate their own deformability and flow velocity
Acknowledgments
This study was supported by the NIH/NINDS. We thank Takahiro Takano, Lulu Xie, Wei Song, Priyanka Pillai, Prishanya Pillai, and Jordana Schmierer for expert technical assistance, and Dan Xue for assistance with illustrations.
Footnotes
Author Contributions
Conceptualization, M.N., J.W., and H.S.W.; Methodology, H.S.W., H.K., I.D.R, N.L., and S.Z.; Software, I.D.R. and H.S.W.; Investigation, M.N., J.W., H.S.W., H.K., N.L., S.Z., Y.W., E.D.M., and A.G.; Resources, A.F.P., K.E.R., and C.X.; Writing – Original Draft, M.N., J.W., and H.S.W.; Writing – Review & Editing, M.N., J.W., H.S.W., S.Z., A.F.P., and I.D.R.; Visualization, M.N., J.W., H.S.W., and S.Z.; Supervision, M.N. and J.W.; Funding Acquisition, M.N. and J.W.
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