Abstract
Experimental and clinical studies indicate that waves of cortical spreading depolarization (CSD) appearing in the ischemic penumbra contribute to secondary lesion growth. We used an embolic stroke model that enabled us to investigate inverse coupling of blood flow by laser speckle imaging (CBFLSF) to CSD as a contributing factor to lesion growth already in the early phase after arterial occlusion. Embolization by macrospheres injected into the left carotid artery of anesthetized rats reduced CBFLSF in the territories of the middle cerebral artery (MCA) (8/14 animals), the posterior cerebral artery (PCA) (2/14) or in less clearly defined regions (4/14). Analysis of MCA occlusions (MCAOs) revealed a first CSD wave starting off during ischemic decline at the emerging core region, propagating concentrically over large portions of left cortex. Subsequent recurrent waves of CSD did not propagate concentrically but preferentially circled around the ischemic core. In the vicinity of the core region, CSDs were coupled to waves of predominantly vasoconstrictive CBFLSF responses, resulting in further decline of CBF in the entire inner penumbra and in expansion of the ischemic core. We conclude that CSDs and corresponding CBF responses follow a defined spatiotemporal order, and contribute to early evolution of ischemic territories.
Keywords: embolic stroke, experimental, focal brain ischemia, laser speckle imaging, spreading depression
Introduction
Propagating waves of depolarization typically referred to as cortical spreading depression (Leao, 1944a) or cortical spreading depolarization (CSD) emerge spontaneously in areas of cerebral cortex surrounding newly developing brain infarcts in animal models of focal ischemia (Hossmann, 1996; Nedergaard and Astrup, 1986), brain trauma (Nilsson et al, 1993; Ozawa et al, 1991), and subarachnoid hemorrhage (Dreier et al, 1998). Moreover, recent clinical studies show that CSD or CSD-like events appear around the site of brain injuries in human patients suffering from acute brain trauma (Strong et al, 2002), intracerebral or subarachnoid hemorrhage (Dreier et al, 2006; Fabricius et al, 2006), and malignant hemispheric stroke (Dohmen et al, 2008). These events, alternatively termed peri-infarct depolarization (PID), augment the mismatch between supplied substrate and energy demand of tissue at risk (Busch et al, 1996; Takano et al, 1996). The number of depolarizations or their cumulative duration is associated with infarct growth (Back et al, 1996; Dijkhuizen et al, 1999; Mies et al, 1993).
A mechanism repeatedly proposed in recent literature as contributing to the devastating effect of CSD in areas around the site of brain injuries is the association of reductions in regional cerebral blood flow (CBF) with the depolarizations. This decreased CBF has been found in models of subarachnoid hemorrhage (Dreier et al, 1998) and focal ischemia (Shin et al, 2006; Strong et al, 2007), and new evidence exists that they may cause secondary ischemic damage in human brains after subarachnoid hemorrhage (Dreier et al, 2009; Iadecola, 2009). In the normally perfused brain, in contrast, CBF increases in response to CSD as already shown by Leao (1944b) in the second of his two memorable articles.
Of considerable interest for the estimation of CSD contribution to infarct growth is the spatiotemporal aspect of the spread of both the depolarization wave and the coupled CBF response to this wave, in particular because this response may be inverted (Dunn et al, 2001; Shin et al, 2006; Strong et al, 2007). One unsolved problem is for instance whether CSD and CBF responses coupled to CSD participate in the evolution of ischemic territories already in the early phase of occlusive stroke. To address this question, we used real-time imaging with laser speckle flowmetry (LSF) covering the dorsolateral aspect of the cortical surface of one hemisphere. The LSF has been proved a surrogate tracker of depolarization waves in earlier work (Dunn et al, 2001; Shin et al, 2006; Strong et al, 2007) and is a semiquantitative but fast measure of dynamic CBFLSF alterations. A modified embolic focal ischemia model in rats generated by intracarotid injection of a macrosphere (Gerriets et al, 2004) allowed remote occlusion and was therefore especially well suited for continuous imaging during the occlusive process.
Materials and methods
Surgical Preparation
All animal procedures were performed in accordance with the German regulations for animal protection and were approved by the local animal care committee and local governmental authorities. Male Wistar rats (n=14) weighing 300 to 360 g were anesthetized with 5% isoflurane and maintained with 2% to 2.5% isoflurane in a gas mixture of 65% nitrous oxide and 35% oxygen. Throughout the surgical procedures and the experiments, rectal temperature was maintained at 37.5°C, with a thermostatically controlled heating pad. The left femoral artery and vein were cannulated to allow continuous monitoring of arterial blood pressure and intermittent injection of drugs as indicated below. To prepare embolization by a macrosphere, a catheter (PE-50) was inserted into the internal carotid artery (ICA) as described elsewhere (Gerriets et al, 2004). In brief, after exposure of the left common carotid artery, ICA, and external carotid artery, the external carotid artery and the pterygopalatine branch of the ICA were ligated. PE-50 tubing filled with heparinized saline and one TiO2 macrosphere (∅ 0.315 to 0.355 mm; BRACE, Alzenau, Germany) was advanced into the ICA up to the A. pterygopalatine and fixed tightly.
Animals were tracheotomized. After pancuronium injection (first bolus 0.6 mg, followed by 0.4 mg/h), artificial ventilation was started and controlled based on blood gas analysis. The left frontal, parietal, and temporal bones of the rat were exposed and thinned out using a dental drill until they were transparent enough to detect the dura mater (Figure 1A). Drilling was performed under continuous saline irrigation to avoid heat injury. The cavity formed yielded a field of view (12 × 7 mm2) that covered a large portion of the dorsolateral cerebral cortex. Paraffin oil was poured into the cavity, and this pool was temperature controlled at 37.0°C using a servo-controlled electrical heating element. Most of the field of view was covered by the territory of the middle cerebral artery (MCA) as confirmed by anatomical studies using post mortem intraarterial Japan ink injection (Figure 1B) in a separate series of experiments not reported here any further.
Laser Speckle Flowmetry
Real-time measurement of CBFLSF has been implemented to study CSD propagation and CSD-associated CBF alterations under normal conditions (Ayata et al, 2004; Hashemi et al, 2009) and in border zones of experimental focal ischemia (Ayata et al, 2004; Hashemi et al, 2009; Shin et al, 2006; Strong et al, 2007). Methodological details have been described, and quantification aspects have been discussed (Dunn et al, 2001; Strong et al, 2006, 2007). In brief, the exposed cortex was illuminated through thinned skull and dura mater with a laser light (laser diode: DL7140-201, 785 nm, 70 mW, Sanyo and laser diode controller: LDC 205B, THORLABS, Newton, NJ, USA) to produce a speckle pattern that was detected with a CCD camera (A602f-2 BASLER, Ahrensburg, Germany). Raw speckle images were acquired with Speckle Contrast Imaging Software (Andrew Dunn, University of Texas at Austin), and speckle contrast images were acquired at a rate of 40 frames/min. To show that CBFLSF is a suitable surrogate marker for CSD, LSF measurements were combined with DC recordings in one animal. The bone in one small spot was removed and an Ag/AgCl electrode was positioned on the exposed dura. The DC potential was recorded with a sampling rate of 250 Hz, whereas CBFLSF was measured in a single region of interest (ROI) near the electrode, showing coincidence of the electrical and CBF alteration (Figure 1F).
Experimental Design
The LSF system (see above) was positioned over the field of view. After collecting baseline images over a period of 5 minutes, ischemia was induced by slow intracarotid injection of a TiO2 sphere in ∼0.2 mL saline and LSF was continued for 3 hours. Visual control of LSF videos allowed differentiation between various types of territorial ischemic transformation depending on embolization in different cerebral arteries as confirmed by post mortem inspection (Figure 1D). The most common type of occlusion was that of the MCA (8/14 animals; see Table 1). As the MCA territory is well represented in the field of view while others are not (Figure 1B), detailed analysis including statistics was restricted to this entity of eight experimental animals. Mean arterial blood pressure, rectal temperature, and the temperature of the paraffin oil pool were continuously monitored and recorded by a data acquisition system (DASY Lab Ver.9, measX, Mönchengladbach, Germany). Blood gases (pH, pCO2, PO2) and blood glucose were only assessed before start and after finishing LSF recording to avoid artifactual LSF imaging. Experiments were terminated by KCl injection (3 mol/L, 1 mL) immediately after these measurements. In nine animals, isoflurane anesthesia (1.5%) was continued throughout the experiments, in five animals, anesthesia was changed to α-chloralose (80 mg/kg/15 min as a bolus injection and 40 mg/kg/h as a subsequent continuous injection) 1 hour before macrosphere injection. In two cases (see Table 1), the experiment was terminated after a shorter period because blood pressure declined suddenly below 70 mmHg. After measurements, the site where the macrosphere was trapped was confirmed by dissection (Figure 1D).
Table 1. Summary of results obtained in 14 rats after single macrosphere injection.
Animal number | Observation time (hours) | Ischemic territory in field of view | Post mortem site of macrosphere | Time point of primary wave appearance after macrosphere injection (minutes) | Total number of CSDs | Mean velocity of CSDs (mm/min) |
---|---|---|---|---|---|---|
1 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 2 | 11 | 3.11 |
2 | 3 | Uncleara | ICA | 5 | 4 | 3.88 |
3 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 18 | 5 | 3.22 |
4 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 6 | 5 | 2.74 |
5 | 3 | Multiple lesion | ICA | Unclearb | Unclearb | — |
6 | 3 | Uncleara | ACA | 2 | 3 | 3.71 |
7 | 3 | PCAO | ICA | 2 | 13 | 3.38 |
8 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 2 | 7 | 4.44 |
9 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 1 | 14 | 3.75 |
10 | 1.4 | MCAO | MCA (MCA/ACA bifurcation) | 2 | 4 | 3.9 |
11 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 1 | 8 | 3.84 |
12 | 3 | MCAO | MCA (MCA/ACA bifurcation) | 1 | 11 | 3.47 |
13 | 3 | Multiple lesion | ICA | Unclearb | Unclearb | — |
14 | 1 | PCAO | ICA | 8 | 2 | 3.61 |
Mean | 4.2 | 8.1c | 3.56±0.96 |
ACA, anterior cerebral artery; CBF, cerebral blood flow; CSD, cortical spreading depolarization; ICA, internal carotid artery; MCAO, middle cerebral artery occlusion; PCA, posterior cerebral artery; PCAO, posterior cerebral artery occlusion; PCOA, posterior communicating artery.
Injection of macrosphere caused CBF reduction, which did not remain consistent throughout the observation period. CBFLSF waves appeared in the field of view.
Ischemic lesions after macrosphere injection were not homogeneous. CBFLSF waves were observed in the field of view but not clearly confined.
Mean of 10 animals observed for 3 hours.
Data Analysis
Image files and video movie files were generated by reconstruction of speckle contrast images using VINCI imaging software (Volume Imaging in Neurological Research, Max Planck Institute for Neurological Research, Cologne, Germany). To investigate the spatial and temporal patterns of CSD and associated CBFLSF changes, 25 ROIs (1.2 × 1.2 mm2) were equally distributed over the cortical field of view labeled A–Y (Figure 1C). Percent changes of CBF were calculated by taking control values averaged over 1.5 minutes before injection of macrospheres as 0% and final values after kill (complete ischemia) as −100%.
Nevertheless, one should take the magnitude of relative flow changes with caution, because factors like unequal thinning of the skull or depth of oil pool have not been corrected for.
Statistics
To test whether MCA occlusion (MCAO) would result in a significant CBF reduction, CBF values for all ROIs (A–Y) at the time points 1, 2, and 3 hours were tested against preischemic control using the one-sample t-test. Resulting P values were corrected for multiple comparisons (25 ROIs × 3 time points=75 tests) using the Benjamini–Hochberg false discovery rate procedure (Benjamini and Hochberg, 1995). α=0.05 was used as significance level in all tests. To test whether development of CBF after 3 hours is influenced by initial CBF reduction, a linear regression analysis was performed with CBF reduction during the first hour as independent variable, and CBF reduction after 3 hours as dependent variable.
To investigate the influence of space and time on CBF reduction, CBF data of all ROIs (A–Y) at all time points (baseline, 5 minutes, 1 hour, 2 hours, and 3 hours) were compared using a two-way repeated measures analysis of variance (ANOVA), with the arc sine square root-transformed data. As tests for normality (Kolmogorov–Smirnov test) and equal variance (Levene median test) failed, a rank transformation was performed before ANOVA. This procedure is suitable for tests of main effects, but inappropriate for testing interactions (Seaman et al, 1994). Another ANOVA was therefore calculated with the original data, where interaction of the factors ‘ROI' and ‘time' was not statistically significant (F(96;576)=1.021; P=0.433). As variance heterogeneity results in an underestimation of type I error, factor interaction was regarded as nonsignificant, and was not tested in the ANOVA on ranks. In the following post hoc multiple comparison procedure (Holm–Sidak method), the least affected ROI (A) and the time point ‘baseline' were used as controls.
Sorting of ROIs according to baseline CBF reduction revealed three groups of high (A–H), middle (I–P), and low (Q–Y) CBF. To test whether the groups were significantly different, a one-way ANOVA was performed with the arc sine square root-transformed mean values (across animals) of each ROI (i.e., n=8 for ‘high,' n=8 for ‘middle,' n=9 for ‘low'). Normality and equal variance were tested using the Kolmogorov–Smirnov test and the Levene median test, respectively. ANOVA was followed by an all pairwise multiple comparison procedure (Holm–Sidak method). A significant difference was detected (F(2;22)=337.02; P<0.001), and post hoc comparison revealed that all factor levels (high, middle, and low CBF) were significantly different from each other. Subsequently, a two-way repeated measures ANOVA was performed with time (base, 5 minutes (i.e., after passage of the first wave), 1 hour, 2 hours, and 3 hours) used as factor 1, and group (low, middle, and high CBF) as factor 2, followed by an all pairwise multiple comparison procedure (Holm–Sidak method).
To evaluate how the development of CBFLSF was influenced by the level of prewave baseline under different conditions (i.e., wave order and height of wave maximum compared with baseline), data were grouped according to four categories: (1) first wave; maximum<base, (2) first wave; maximum>base, (3) subsequent waves; maximum<base, and (4) subsequent waves; maximum>base. Subsequently, linear regression analyses were performed separately for each group, with ‘base' as the independent and ‘effect' as the dependent variable. To compare the slopes of regression lines, the slope (b) of every data point (base xi; effect–base yi) was calculated using the formula
with x̄ being the mean of base values, and ȳ the mean of effect values. Slopes of the four groups were compared using the Kruskal–Wallis one-way ANOVA on ranks, because data were not normally distributed. Post hoc pairwise multiple comparison was performed using Dunn's method.
Results
Already during online CBFLSF imaging, and also retrospectively during analysis of LSF-derived videos covering the full-observation period of 3 hours, three principal features of dynamic CBFLSF alterations were observed: (1) a fast, almost immediate gradual decline of CBFLSF after macrosphere injection generating ischemic foci in the arterial territories of the MCA (8/14 animals) or posterior cerebral artery (PCA, 2/14); in other cases (4/14), the attribution to arterial territories was less clear, and eventually, multiple ischemic lesions developed; (2) a primary propagating wave of CBFLSF alteration originating at the border of the ischemic territory soon after the first CBFLSF decline (delay after macrosphere injection: 4.2 minutes) spreading concentrically with a velocity of around 3.4 mm/min and crossing the entire exposed cortex; and (3) multiple subsequent, secondary waves of CBFLSF alteration propagating with similar velocity but taking a circumferential course around the freshly created ischemic territory by avoiding the core region and sometimes regions most distant to the ischemic core. Temporally, secondary waves were distributed almost equally over the 3-hour observation period.
The CBF waves turned out to be quite similar to those reported earlier in other models of focal ischemia in lissencephalic brains of mice and gyrencephalic brains of cats (Shin et al, 2006; Strong et al, 2007). To most easily identify the dynamic nature of the three-mentioned processes, we recommend watching Supplementary Videos 1–4, showing respective three principal features before going into details of the results.
Effects of Embolic Occlusion on CBFLSF
The most frequent effect of macrosphere injection was the immediate evolution of an ischemic lesion in the MCA territory covering a significant portion of the field of view (Table 1; see also Supplementary Video 1). As other types of territorial ischemic transformations were less represented or less clear in their spatial dispersion, forming single or multiple smaller lesions in the field of view (Table 1; see also Supplementary Video 2 displaying the evolution of an ischemic lesion in the territory of the PCA), we restricted formal analysis to occlusions of the MCA. Region of interest analysis of 25 ROIs (Figure 1C) showed gradual decline of CBFLSF, with lowest values in the most lateral and highest values in medial portions of the field of view. ANOVA confirmed that the spatial factor ‘ROI' significantly influenced CBF reduction (F(24;576)=23.24; P<0.001), and post hoc analysis revealed lower CBFLSF values in the three lateral rows of ROIs (I–Y) compared with the medial ROIs (B–H). The gradual decline of CBFLSF is best seen in line plots of mean CBFLSF values taken for individual ROIs over the whole observation period (Figures 2A and 2B) and in sequential stills of videos (Figure 2C). Superimposed waves of CBFLSF appearing repetitively in these line plots document multiple appearance of CSD after MCAO. Interestingly, all ROIs showed a significant decline (one-sample t-test against baseline) of mean CBFLSF averaged over the first hour after MCAO (Figures 3A and 3B), even though anterior, medial, and posterior ROIs were not attributable to the MCA territory. This general CBFLSF reduction persisted during the 3-hour observation period (Figure 3C). A weak, even though significant tendency existed for partial recirculation within the 3-hour time frame, being more prominent in ROIs with severe CBFLSF reduction in the MCA territory (Figure 3D, see also Figures 2A and 2B).
Concentric Propagation of First CBFLSF Wave After Middle Cerebral Artery Occlusion
The first CBFLSF wave appeared in most instances very early after arterial occlusion, within or right after the first steep fall of CBFLSF (Table 1). This primary wave was observed in all experiments. It propagated always concentrically, originating from the core of the arising ischemic lesion and crossing the whole field of view. Sequential still images taken from a Laser Speckle video showing the propagation of a primary wave (Figure 4A) illustrate that a front of reduced perfusion (blue) precedes a hyperemic tail of the wave (red). The baseline image taken just before the onset of the first wave ignores the initial reduction of CBFLSF resulting from MCAO to better visualize the effects of the wave (see also Supplementary Video 3). After passage of this first CBFLSF wave, the ischemic lesion appeared intensified as shown by the ischemic transformation superimposed on the primary ischemic focus (region encircled in the last still in Figure 4A by dashed line) and also by the continued decrease of CBFLSF in ROIs in the core-like ROI ‘V' (see Figure 4A, line plot). These gradual differences in CBFLSF response patterns become more evident when looking at chart recordings of all 25 ROIs in an individual animal spatially arranged corresponding to ROI arrangement on the cortical surface: monophasic reductions of CBFLSF dominated in core regions (in example presented in Figure 5A, ROIs P–S, V–Y), whereas in border zones of the ischemic focus, biphasic responses (Figure 5A, ROIs A–F, I–O, T–U) or, even more peripherally, monophasic increases of CBFLSF (Figure 5A, ROIs G–H) were characteristic.
Analysis of these response patterns was systematically performed as shown in Figure 6A: separate components of CBFLSF waves (base, minimum, maximum, and effect) were identified for individual waves and related to preischemic control levels of CBFLSF. This analysis revealed that after passage of the primary wave, CBFLSF decreased further in regions with most severe primary ischemia (Figure 6B). In the ‘low-CBF' group (ROIs Q–Y), CBFLSF was significantly reduced after the passage of the first wave and was still significantly lower than prewave baseline after 3 hours (main effect of factor time: F(4;88)=11.5, P<0.0001; all time points were significantly different from baseline). This secondary CBFLSF reduction was possibly due to lack of a phase of compensatory CBFLSF increase above prewave baseline, reflected by a positive regression between base and effect (see Figure 6C, regression ‘maximum<base'). In regions more distant from the core, in contrast, CBFLSF increased after wave passage, indicated by a negative regression between base and effect (see Figure 6C, regression ‘maximum>base').
Circumferential Propagation of CBFLSF Waves in the Later Course of Middle Cerebral Artery Occlusion
Subsequent to the primary CBFLSF wave, multiple waves continued to appear over the observation period of 3 hours in all animals with MCAO (Table 1). The propagation pattern, however, changed considerably: CBFLSF waves typically came into the field of view from one edge and travelled circumferentially around the freshly developed ischemic core, or they originated near the core propagating then also circumferentially (see Supplementary Video 4). Sequential still images taken from a Laser Speckle video (Figure 4B) illustrate that despite the change in direction of travel, secondary waves resembled the primary waves comprising a front of reduced perfusion (blue) followed by a hyperemic tail of the wave (red). The spatial dispersion of subsequent waves differed insofar as they did not propagate in the ischemic core, if CBFLSF reduction was severe. Therefore, a smaller number of ROIs was crossed by the waves. Further analysis of CBFLSF patterns in circumferential waves revealed spatial differences in proximity to the core: near to the core, monophasic reductions of CBFLSF were dominant (for example as presented in Figure 5B, ROIs P–Q, J–K), whereas with increasing distance to the core, waves became biphasic (Figure 5B, ROIs S–U, I, M–O, A–D) or showed monophasic CBFLSF increases (Figure 5B, ROIs E–H). Thus, response patterns of secondary waves showed a similar, though less pronounced tendency to spatially alter CBFLSF as observed for primary waves: Secondary waves also induced further decreases of CBFLSF in ROIs near the ischemic focus, as indicated by a positive regression between base and effect (see Figure 6D, regression ‘maximum<base'). In regions more distant from the core, CBFLSF instead increased after wave passage, as reflected by a negative regression between base and effect (see Figure 6D, regression ‘maximum>base'). However, the increase of CBFLSF after secondary waves was less pronounced than after primary waves, leading to a significantly lower slope of the regression line for secondary waves.
Discussion
The central finding in this study was the differentiation between primary and subsequent, secondary waves of cortical blood flow alteration associated with CSD in the area surrounding freshly generated focal ischemic lesions in the ‘macrosphere' model of MCAO in rats: primary waves propagated concentrically from the lesion outwards into healthy tissue crossing almost the entire cortex, whereas subsequent waves traveled circumferentially around the lesion, and the dispersion of secondary waves was more or less restricted to the lesion border. The second finding of relevance relates to the use of LSF as a measure of regional blood flow: CBFLSF waves were polymorphic as described for several models of focal ischemia (Luckl et al, 2009; Shin et al, 2006; Strong et al, 2007). Both primary and secondary types of CBFLSF waves contributed to the evolution of the ischemic lesion, the primary having more impact in the observed early phase.
A major benefit of using the ‘macrosphere' model in combination with LSF was its suitability to remotely occlude a cerebral artery (Gerriets et al, 2004) allowing continuous observation in real time: (1) the consequences of macrosphere arrival, (2) the ischemic focus in status nascendi, and (3) the immediate onset of multiple CBFLSF wave passages over significant portions of cerebral cortex. The model used did not allow observation of the whole circumference of the lesion as previously shown by our group in a ‘distal' MCAO model with coagulation of a distal branch of the MCA that enabled us to observe cyclic repetitive propagation of PID-associated CBFLSF waves around the ischemic focus (Nakamura et al, 2010). In the ‘distal' MCAO model, however, the transition from preischemic to ischemic conditions was not available, and therefore, a differentiation between primary and secondary waves was impossible.
Laser speckle imaging was introduced in 2001 for the study of CBF (Dunn et al, 2001), and has been applied since to examine CBF alterations related to functional brain activation and spreading depression in physiological conditions (Ayata et al, 2004; Dunn et al, 2003; Durduran et al, 2004; Obrenovitch et al, 2009; Sakadzic et al, 2009), as well as to focal cerebral ischemia and associated PIDs (Luckl et al, 2009; Shin et al, 2006, 2007; Strong et al, 2007). Despite the fact that quantification may be obtained under optimal experimental conditions (Strong et al, 2006), we used LSF as a relative measure implementing a scale that took preischemic control values before macrosphere injection as zero, and post mortem values as −100%. Even though the linearity of this scale remains obscure, the data obtained were convincing with regard to the use of LSF as a tool to (1) dynamically examine the evolution of an ischemic focus, (2) track CSDs, and (3) distinguish between different patterns of CBF transients in response to CSD.
The LSF allowed observation of the rapid evolution of ischemic foci: in the eight animals developing a typical spatial pattern of MCAO in our study, the ischemic territory began to form only seconds after the macrosphere got trapped (see Supplementary Video 1). Only in these animals did post mortem analysis reveal that the site of macrosphere trapping was indeed the MCA/anterior cerebral artery (ACA) bifurcation. A rather large portion of animals (6/14) did not develop clear spatial patterns of ischemia. In these animals, macrospheres were mostly trapped in the ICA. The high rate of failure to produce a clear ischemic focus may be regarded disadvantageous and is most probably due to our use of a single rather than four macrospheres, as was the case in former studies using this model (Gerriets et al, 2004). The time point of occlusion seemed to us less well defined, with injection of four macrospheres even though the incidence of successful occlusion is presumably higher and infarction larger. In our study, however, we were particularly interested in the temporal relationship between onset of ischemia and appearance of the first wave as compared with subsequent waves of CSD-related CBF transients and thus wanted to avoid ambiguity in the temporal generation of the ischemic focus derived from variable time points of occlusion because of sequential trapping of multiple macrospheres in various arterial branches.
Regarding the general effects of MCAO, CBFLSF decreased gradually, the most lateral ROIs showing most severe reductions. It was remarkable that small but consistent decreases of CBFLSF were even observed in medial ROIs attributable to the ACA territory and in occipital ROIs attributable to the PCA territory. This might reflect a condition similar to the ‘reversible cerebral vasoconstriction syndrome' described in human patients (Ducros and Bousser, 2009), a general vasoconstriction, which can be caused by mechanical damage to major arteries.
Surprisingly, in most animals including not only those with clear signs of MCAO but also those with ICA or ACA involvement, primary CBFLSF waves developed rapidly within the first few minutes after macrosphere injection appearing in the field of view of the laser speckle system. These waves turned up during or immediately after the first occlusive reduction of CBF. In case of MCAO, primary CBFLSF waves always propagated concentrically originating in the most lateral ROIs spreading concentrically in medio–occipito–frontal direction. Waves typically crossed all 25 analyzed ROIs, and we suspect that they spread over the entire cortex. Concentric wave propagation of CSDs has been described in rats and cats under physiological conditions after induction with high potassium (Farkas et al, 2008; Smith et al, 2001; Tomita et al, 2002). In focal ischemia, in contrast, rostral-caudal or circumferential propagation around the ischemic core seems to be the predominant pattern (Hartings et al, 2003; Luckl et al, 2009; Nakamura et al, 2010). Only in one study in cats, was radial propagation from the core to the periphery showed during the early phase after proximal MCAO (Nakamura et al, 2010). As concentric propagation seems to be restricted to the initial phase of focal ischemia, tissue conditions might still be quite normal early after occlusion and comparable to the conditions encountered during artificial CSD induction in physiological conditions.
The form of the primary waves was polymorph as described for other models of focal ischemia (Luckl et al, 2009; Strong et al, 2007; Sukhotinsky et al, 2008), but not consistent throughout the course of spread. Rather, waves started as predominantly monophasic hypoperfusion waves, and as they travelled into the border zone of the ischemic focus, they became biphasic, with a phase of hypoperfusion preceding a hyperemic phase. Thereafter, in the periphery of the focus, they became almost purely hyperemic and thus again monophasic. This transition took place in watershed zones between arterial territories of the MCA on the one side and those of the ACA and PCA on the other. For primary waves, we assume that the transition of morphology is characteristic for their travel through changing conditions into the periphery of the developing focus, and they may therefore represent an excellent model to study underlying mechanisms of normal or inverted coupling of blood flow to spreading depolarization as first described by Dreier et al (1998) in a model of subarachnoid hemorrhage. Furthermore, they may indeed participate in the maturation of zonal gradation of ischemic foci: in inner zones near the wave origin exhibiting most severe ischemic reductions of CBF, these hemodynamic transients cause a further decline of CBF compared with outer zones because of the fact that compensatory hyperemic portions of the transients are missing here while they are pronounced in outer zones. To illustrate this phenomenon, we have separated ROIs with intact compensatory abilities (condition ‘maximum>base') from those where compensation is no longer possible (condition ‘maximum<base'), and performed separate regression analyses between the variables ‘base' (the prewave baseline) and ‘effect' (CBFLSF level after passage of the wave) with the two groups (see Figure 6C). The compensatory mechanisms of intact tissue are impressively shown by the negative slope of the regression line in the condition ‘maximum>base,' indicating that the lower the initial CBFLSF, the more effective the reperfusion after the first CSD. In contrast, in the group ‘maximum<base,' the regression was positive, demonstrating that the lower the initial CBFLSF, the stronger its further decline. As a result, the demarcation between inner and outer zones is enhanced after the passage of primary waves.
In animals developing MCAO, the next CBFLSF waves after primary concentric waves already showed a completely different spatial course of propagation: they travelled around the core region, the main direction being rostral-caudal or reverse, respectively, clockwise or counterclockwise. This spatial pattern of CBFLSF wave propagation remained predominant for subsequent waves throughout the 3-hour observation period. Our finding indicates that under pathophysiological conditions like those developing in the ischemic border zone after arterial occlusion, the basis for propagation of PIDs or CBFLSF waves substantially changes soon after MCAO leading to the change of the spatiotemporal propagation pattern. What are the essential alterations of tissue conditions that may affect the spatiotemporal pattern of spread? Despite substantial efforts, the mechanism of CSD or PID propagation has never been convincingly identified. Two major hypotheses have been proposed, one postulating extracellular mechanisms of diffusion of substances like potassium or glutamate, which are involved in the process of depolarization and appear in rather high extracellular concentrations during CSD, the other suggesting intercellular propagation of substances like potassium through gap junctions, either between neurons or between glial cells (Somjen, 2001). In core regions of evolving ischemic foci, substances like potassium and glutamate are excessively liberated shortly after anoxic depolarization and presumably diffuse into the surrounding border zones (Shimada et al, 1989). Thus, if CSD induction occurs at some time point at the edge of the ischemic core, this depolarization will cause additional release of potassium and glutamate and may thereby easily initiate, presumably in a cascade-like manner, depolarization around the whole circumference of an ischemic border zone, where potassium and glutamate concentrations are already elevated by diffusion from the core—a process that takes some time, possibly the time elapsing between first and subsequent waves. We assume that it is this time point that marks the transition of cortical tissue into conditions of the ischemic penumbra. Extracellular potassium transients in particular were reported already in the 1970s to characterize such conditions (Branston et al, 1977). The ischemic penumbra, therefore, is perhaps primed or preconditioned for preferential CSD/PID propagation as soon as anoxic depolarization has occurred in the core region resulting in the liberation of substances like potassium and glutamate and diffusion of these substances into this region. As a consequence, rostral-caudal or circumferential propagation around the ischemic core seems to emerge as the predominant pattern of CSD/PID propagation in focal ischemia of cats and rats (Hartings et al, 2003; Luckl et al, 2009; Nakamura et al, 2010). Even more convincingly, we have recently been able to show in rats in a model of occlusion of distal branches of the MCA that CBFLSF waves circle not only once but multiple times around an ischemic lesion that was substantially smaller than in the model used in this study so that the whole circumference of the lesion could be visualized by LSF (Nakamura et al, 2010). Regarding the dispersion of primary and secondary CBFLSF waves, it is also interesting to note that only primary waves appeared in almost all ROIs covering perhaps the whole hemisphere, whereas secondary CBFLSF waves did not appear in the most lateral ROIs (see Figure 5) representing core regions of the MCAO. It is well known that CSDs do not propagate in injured or infarcted tissue (Somjen, 2001), and therefore we consider ROIs without a secondary wave ischemic core. It seems obvious that not only penumbra but also core conditions evolve spatially in a highly dynamic manner during this early stage of arterial occlusion, and it should be mentioned in this context that other mechanisms like increased oxygen extraction in ischemic border zone regions (Heiss et al, 1994) participate in this spatially transitional phase.
With respect to the emergence of a gradual decline in CBF in the ischemic territory, secondary CBFLSF waves showed similar polymorphism as that found for primary waves: in the inner penumbra near the ischemic core, monophasic reductions of perfusion were dominant, whereas monophasic increases of CBF were seen in most peripheral ROIs. Biphasic responses with decreases followed by increases of CBF were mostly observed in the outer penumbra. Similar polymorphism has been documented in other models of focal ischemia in cats and rats (Luckl et al, 2009; Shin et al, 2006; Strong et al, 2007). It seems that in outer zones, anastomoses between arterioles of the ischemic MCA territory and the neighboring ACA and PCA territories work efficiently to allow CBF elevation through collateral channels, whereas in inner zones, this type of coupling of CBF to depolarization seems to be more and more reversed. As a mechanism of inverted coupling during CSD, nitric oxide synthase inhibition in the presence of raised potassium has been discussed (Dreier et al, 1998), indicating that under physiological conditions, nitric oxide mediates increases of cerebral perfusion coupled to CSD. Even though the effect of secondary CBFLSF waves on a further reduction of CBF in inner zones of the penumbra seems rather small from our results (see Figure 6), it should be emphasized that multiple CSDs/PIDs are to be expected in the course of focal ischemia and stroke resulting in additive deleterious effects, in particular, if clusters of CSD/PID appear (Bosche et al, 2010; Dohmen et al, 2008; Dreier et al, 2006). In SAH patients, for example, we have recently shown that within clusters of CSD, oxygen availability decreases considerably (Bosche et al, 2010; Dohmen et al, 2008; Dreier et al, 2006). Similarly, extracellular glucose availability may decrease after CSD passage, which even occurs under almost physiological conditions (Hashemi et al, 2009).
We conclude that the primary CSD or CBFLSF wave after an ischemic stroke is most relevant in terms of initially separating tissue compartments where compensatory mechanisms are still possible from those where CBF reduction can no longer be compensated. In contrast to the primary wave, which travels across the whole hemisphere, the secondary waves mostly remain in the ischemic border zone and contribute to its differentiation. The CSDs therefore seem to act as a trigger mechanism of infarct evolution.
The authors declare no conflict of interest.
Footnotes
Supplementary Information accompanies the paper on the Journal of Cerebral Blood Flow & Metabolism website (http://www.nature.com/jcbfm)
Supplementary Material
References
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