Norepinephrine links astrocytic activity to regulation of cortical state

Norepinephrine links astrocytic activity to regulation of cortical state

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ABSTRACT Cortical state, defined by population-level neuronal activity patterns, determines sensory perception. While arousal-associated neuromodulators—including norepinephrine (NE)—reduce


cortical synchrony, how the cortex resynchronizes remains unknown. Furthermore, general mechanisms regulating cortical synchrony in the wake state are poorly understood. Using in vivo


imaging and electrophysiology in mouse visual cortex, we describe a critical role for cortical astrocytes in circuit resynchronization. We characterize astrocytes’ calcium responses to


changes in behavioral arousal and NE, and show that astrocytes signal when arousal-driven neuronal activity is reduced and bi-hemispheric cortical synchrony is increased. Using in vivo


pharmacology, we uncover a paradoxical, synchronizing response to Adra1a receptor stimulation. We reconcile these results by demonstrating that astrocyte-specific deletion of _Adra1a_


enhances arousal-driven neuronal activity, while impairing arousal-related cortical synchrony. Our findings demonstrate that astrocytic NE signaling acts as a distinct neuromodulatory


pathway, regulating cortical state and linking arousal-associated desynchrony to cortical circuit resynchronization. SIMILAR CONTENT BEING VIEWED BY OTHERS DISTINCT ASTROCYTIC MODULATORY


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ASTROCYTES REGULATED BY LOCUS COERULEUS Article Open access 03 April 2024 NETWORK-LEVEL ENCODING OF LOCAL NEUROTRANSMITTERS IN CORTICAL ASTROCYTES Article Open access 17 April 2024 MAIN


Patterns of neural activity in the awake cortex are variable1, ranging from states of highly synchronized neuronal activity during periods of low arousal, to states of desynchronized


activity during high-arousal periods such as whisking2 and running3. These cortical states can be identified by electrophysiological activity: synchronized cortical states display greater


low-frequency (LF) oscillations and reduced high-frequency (HF) oscillations than desynchronized states4. While HF oscillations are important for processing of incoming information5, LF


oscillations during the wake state are less well characterized. Generally described within a 2–10 Hz range2,6,7, wakeful LF power differs substantively from cortical activity patterns during


sleep2, indicating a unique role for synchronized cortical states in awake animals. One role of waking cortical synchrony may be to modulate sensory responses to external stimuli. Increased


LF power is associated with reduced neuronal gain6 and broader tuning8 in sensory cortex, as well as diminished behavioral performance on sensory perception tasks3,7,8. The mechanisms by


which cortical state is regulated, and how the cortex becomes sensitized to external stimuli, are well studied. One central mechanism is signaling by norepinephrine (NE), which regulates a


primary hallmark of behavioral arousal—pupil diameter9—and alters the firing properties of cortical neurons leading to desynchronized cortical activity10,11. However, while the


desynchronizing effects of NE are well known, mechanisms that increase waking synchrony are less clear. A full understanding of mechanisms that regulate awake cortical synchrony will be


necessary to explain fluctuations in perception and behavior. Neurons are not the only NE-responsive cell types in the cortex12,13. Astrocytes, a non-neuronal cell type abundant throughout


the cortex, respond to NE with robust calcium (Ca2+) signaling14,15,16,17,18,19. However, astrocyte Ca2+ has also been linked to increased cortical synchrony when NE signaling is low,


including during sleep20 and under anesthesia21. In this Article, we aimed to resolve the disparity between an astrocytic role in sleep generation and their activation by NE and


desynchronizing stimuli such as movement. We hypothesized that NE-specific astrocytic signaling might act as a mechanism that regulates NE-driven cortical desynchrony and restores cortical


synchrony following changes in arousal. Here we use in vivo, two-photon (2P) Ca2+ imaging to show that astrocytes in mouse visual cortex respond proportionally and with temporal specificity


to changes in arousal and NE, positioning astrocytes as a local feedback mechanism to the effects of arousal. In agreement with this hypothesis, NE-driven astrocyte Ca2+ signaling occurs


alongside reductions in arousal-associated neuronal activity. Using in vivo local field potential (LFP) recordings, we further show that arousal-driven astrocyte Ca2+ activity occurs at


transitions from cortical desynchrony to synchrony, and that this relationship is dependent on NE signaling. Pharmacological stimulation of Adra1a receptors counterintuitively increases


wakeful cortical synchrony, and astrocyte-specific removal of _Adra1a_ enhances total and arousal-driven neuronal activity, while impairing arousal-related cortical synchrony. Our results


directly link astrocytic NE receptors to cortical state regulation. We thus identify NE signaling to astrocytes as a new circuit mechanism by which astrocytes act as sensors of NE changes


and synchronize the cortex in response to arousal. RESULTS ASTROCYTE CA2+ CORRELATES WITH INCREASES IN PUPIL DIAMETER To first determine whether astrocyte Ca2+ activity is dynamically


modulated by arousal, we carried out in vivo, 2P Ca2+ imaging in visual cortex of awake, head-fixed mice while simultaneously recording pupil diameter and running speed (Fig. 1a). We


expressed the Ca2+ indicator GCaMP in cortical astrocytes under the GfaABC1D promoter and used the Astrocyte Quantitative Analysis (AQuA) toolkit22 to accurately capture dynamic fluorescent


astrocyte signals, even from spatially overlapping events (Extended Data Fig. 1a,b). We extracted fluorescence traces from all AQuA-detected Ca2+ events and found that movement was


accompanied by large increases in astrocyte Ca2+—as well as increases in arousal indicated by pupil dilation—consistent with previous reports6,14,16,23,24 (Fig. 1b, left). Even during


stationary periods, astrocyte Ca2+ activity was accompanied by concurrent and proportional fluctuations in arousal (Fig. 1b, right). Population astrocyte Ca2+ activity was better correlated


with pupil diameter (0.51 ± 0.09) than running speed (0.21 ± 0.07) when comparing across mice (Fig. 1c, top, _n_ = 6 mice) or using hierarchical bootstrapping (HB, Fig. 1c, bottom). In


addition, individual astrocyte Ca2+ events correlated better with arousal compared with either speed- or time-shuffled data (Extended Data Fig. 1c, left). Most Ca2+ events (9,597/11,674;


82.2%) exhibited a maximal cross-correlation with pupil diameter within 10 s and a short (0.32 ± 0.01 s standard error of the mean (s.e.m)) lag, consistent with arousal driving astrocyte


activity (Extended Data Fig. 1c, right). Our analysis indicates that arousal contributes to astrocyte Ca2+ beyond its association with movement. However, cortical activity reflects both


absolute pupil diameter23 and relative changes in pupil diameter24. To investigate whether astrocytes sense absolute levels of arousal, we binned the pupil diameter into deciles (Fig. 1d,


left), and calculated the average Ca2+ fluorescence in each. Astrocyte Ca2+ dynamically varied with pupil diameter only when the pupil was ~40–80% of maximum diameter (Fig. 1d, right, and


Supplementary Table 1). This range matched the overlap in pupil diameter found between stationary and movement periods (Extended Data Fig. 1d), indicating this relationship was a function of


movement, and suggesting that absolute pupil diameter did not adequately explain the relationship between arousal and astrocyte Ca2+. To test whether relative changes in pupil diameter were


linked to astrocyte Ca2+ responses, we calculated an event-triggered average relative to the start of movement. As expected, we found that pupil diameter and—with a short delay—astrocyte


Ca2+ increased around movement onset (Fig. 1e). We then asked which behavioral variables best explained movement-evoked astrocyte Ca2+ activity (Fig. 1f–h). We found that speed was a poor


predictor of the maximal astrocyte Ca2+ fluorescence (Fig. 1f, left) as previously reported16, as was the relative change in speed (Fig. 1f, right). In addition, absolute pupil diameter


following movement had a weak correlation with astrocyte Ca2 fluorescence, indicating that, even during behavioral state changes, absolute pupil diameter is a poor predictor of astrocyte


responses (Fig. 1g, left). In contrast, the relative change in pupil diameter explained a substantial portion of the astrocyte Ca2+ response to movement, indicating that astrocytes are


specifically sensitive to relative changes in arousal (Fig. 1g, right). We further dissociated the effects of movement and arousal on astrocytes by separating behavioral state periods


(Extended Data Fig. 1e). The relationship between astrocyte Ca2+ and increases in pupil diameter persisted during stationary periods (Fig. 1i–j), even though pupil diameter changes were


smaller (Extended Data Fig. 1f). These results demonstrate that astrocytes are sensitive to smaller changes in arousal than previously recognized. We also wondered whether changes in arousal


could explain the timing of astrocyte Ca2+ activity. We noticed that astrocyte Ca2+ peaked with pupil diameter around movement offset (Fig. 1k) and the time to maximum pupil diameter was


strongly correlated with the time to peak astrocyte activity (Fig. 1l). Both were also dependent on the duration of the movement bout (Extended Data Fig. 1g). When examining all astrocyte


Ca2+ events, onsets occurred more often during dilation and offsets during constriction (Fig. 1m). These findings indicate that changes in arousal shape the timing and level of astrocyte


Ca2+ activity. PHASIC INCREASES IN NE PRECEDE ASTROCYTE CA2+ NE is a key driver of both changes in pupil diameter and brain activity25. While recent work suggests that astrocytes


preferentially respond via Ca2+ to “multi-peaked” NE axonal activity15, the impact of behavioral state has not yet been considered. To determine the relationship between NE and astrocyte


Ca2+ activity, we simultaneously expressed a fluorescent sensor of NE, GRABNE26, in cortical neurons under the h-syn promoter and the Ca2+ indicator jRGECO1b in cortical astrocytes under the


GfaABC1D promoter (Fig. 2a and Supplementary Video 1). Examining the raw GRABNE fluorescence, we saw reductions in fluorescence that matched changes in background vasculature, independent


of indicator expression (Extended Data Fig. 2a). Our 2P imaging paradigm was not compatible with techniques to directly measure hemodynamic effects such as reflectance imaging and


blind-source separation27. Therefore, we developed a method to approximate and compensate for hemodynamic signals in 2P imaging (Extended Data Fig. 2b and Methods). To further limit


hemodynamic contamination, we took the mean of the corrected GRABNE signal, excluding highly contaminated or artifactual pixels (Extended Data Fig. 2c). As our methodology only approximates


hemodynamic artifacts and does not account for possible hemodynamics effects from excitation or out-of-plane GRABNE fluorescence, we next sought to confirm the accuracy of our methodology.


We found our corrected GRABNE signal showed little correlation with vasculature or hemodynamically contaminated regions (_r_ < 0.2) but correlated well with regions that had active GRABNE


signal (Extended Data Fig. 2d). To further validate our methodology in an unbiased manner, we correlated individual pixels with pupil diameter (Extended Data Fig. 2e) and found the


corrected GRABNE signal linearly correlated with pupil diameter-related pixels suggesting our method reflects GRABNE signal that occurs from pupil-related increases in NE while reducing


hemodynamic effects (Extended Data Fig. 2f). Using our corrected GRABNE signal, we found that GRABNE fluorescence matched changes in pupil diameter and astrocyte Ca2+ activity, although the


GRABNE showed a slow decay, similar to previous reports15 (Fig. 2b, left). This relationship persisted even during stationary periods (Fig. 2b, right). The slow GRABNE decay was reflected in


the power spectrum, which showed an inverse relationship with frequency (Fig. 2c). Slow (0.01–0.03 Hz) GRABNE fluctuations had more power than the empirically fit 1/_f_ relationship,


suggesting long-lasting fluctuations in “tonic” NE predominate the GRABNE signal. To confirm the link between GRABNE and arousal, we examined the cross-correlation between pupil diameter and


GRABNE. We found a positive correlation between GRABNE and spontaneous changes in pupil diameter (_r_ = 0.13, Fig. 2d), similar to that previously described for cortical NE axons28.


However, the maximum cross-correlation was broad and continued for at least 20 s after the pupil diameter (Fig. 2d, left). Further, unlike what has been reported for NE axons28, GRABNE


showed poor cross-correlation (_r_ = 0.04) with the derivative of pupil diameter (Fig. 2d right, and 2e). These results suggest that cortical GRABNE dynamics best report arousal level rather


than changes in arousal, and may substantively differ from the activity pattern of the underlying NE axons. We next quantified the relationship between GRABNE and astrocyte Ca2+ activity.


We found a positive, broad correlation (_r_ = 0.17) between the two (Fig. 2f, left), with GRABNE preceding astrocyte Ca2+ (−5.7 ± 3.1 s delay, Fig. 2f, right) and GRABNE showing a similar


link to astrocyte Ca2+ as arousal (Fig. 2g). Although slow NE fluctuations predominated our GRABNE signal (Fig. 2c), we also noticed phasic increases in NE (Fig. 2h, left, triangles). We


segregated phasic NE peaks by amplitude (Fig. 2h, left, triangles) and saw that larger phasic GRABNE activity was also longer lasting (Fig. 2h, right, and Supplementary Table 2). We then


examined how astrocyte Ca2+ changed following phasic NE activity. We saw that large (≥2 standard deviations (s.d.)) phasic changes in NE preceded prolonged increases in astrocyte Ca2+ (Fig.


2i–j, left, and Supplementary Table 3, left), while small increases in GRABNE co-occurred with proportional increases in astrocyte Ca2+ (Fig. 2i, right). These increases were observed even


with smaller (1 s.d.) changes in NE (Fig. 2j, right, and Supplementary Table 3, right). These results suggest astrocytes dynamically respond to phasic changes in NE, in both the duration and


amplitude of their Ca2+ signaling. We also calculated the event-triggered average GRABNE signal relative to astrocyte Ca2+ events and confirmed that GRABNE increased before astrocyte Ca2+,


and peaked shortly after astrocyte Ca2+ signaling had begun (Fig. 2k). This relationship was true for both astrocyte Ca2+ events during movement (Fig. 2k, left) and stationary periods (Fig.


2k, right). In sum, these results indicate that astrocytes are sensitive to changes in NE across behavioral states. To corroborate these findings, we performed freely moving, dual-color


fiber photometry recordings of GRABNE and astrocyte Ca2+ (Extended Data Fig. 3a) and saw similar GRABNE dynamics (Extended Data Fig. 3b,c). To confirm the relationship between NE and


astrocyte Ca2+, we used tail lifts to evoke startle responses14, and saw expected increases in both GRABNE and astrocyte Ca2+ (Extended Data Fig. 3d). The GRABNE signal began increasing


before astrocyte Ca2+ and persisted after the startle response (Extended Data Fig. 3e). These results further support the hypothesis that astrocytes respond to phasic increases in NE.


ASTROCYTE CA2+ MAY REDUCE AROUSAL-DRIVEN NEURONAL ACTIVITY We next wondered how arousal-mediated changes in nearby neurons relate to astrocyte Ca2+ activity, as arousal also strongly


modulates neuronal activity6,24,29. To answer this, we expressed hSyn-GCaMP6f in neurons and GfaABC1D-jRGECO1b in astrocytes to record the Ca2+ activity of both cellular populations


simultaneously (Fig. 3a,b and Supplementary Video 2). We found that astrocyte and neuronal Ca2+ fluctuated together along with movement and pupil diameter (Fig. 3c). The average fluorescence


of neurons and astrocytes were maximally correlated with no time shift, a relationship enhanced during movement (Fig. 3d, black, _r_ = 0.46 ± 0.06) compared with stationary periods (Fig.


3d, gray, _r_ = 0.34 ± 0.04). We next investigated how astrocyte Ca2+ relates to arousal-driven neuronal activity specifically. To do this, we used principal component (PC) analysis to


identify the PC of neuronal activity most correlated with arousal (arousal PC)29. We found that the arousal PC of neuronal activity (Fig. 3e, top, red line) often better matched the pupil


diameter (Fig. 3e, top, light gray) than the mean neuronal activity (Fig. 3e, top, dark gray), probably due to the variability in neuronal responses to arousal (Fig. 3e, bottom). In


agreement with previous work29, we found that the arousal PC was usually PC1 (Fig. 3f, gray, 28/35 recordings). Furthermore, we found that average astrocyte Ca2+ activity (Fig. 3g, left,


magenta) was better correlated with pupil diameter than average neuronal Ca2+ activity (Fig. 3f, left, gray). This relationship was reversed when using the arousal PC of astrocyte (Fig. 3g,


right, magenta) and neuronal (Fig. 3g, right, gray) activity instead. The arousal PC consistently reflected arousal-associated activity better than using mean fluorescence for neurons (Fig.


3h, gray dots) but not for astrocytes (Fig. 3h, magenta dots), suggesting that astrocytic responses to arousal are best characterized by a consistent increase reflected in the mean


fluorescence while neuronal responses are best captured by describing the variability in neuronal activity using PC analysis. We next looked at changes in astrocyte Ca2+ and arousal-driven


neuronal activity with arousal. We found that, with both movement (Fig. 3i, top) and stationary increases in pupil diameter (Fig. 3i, bottom), arousal-associated neuronal activity (Fig. 3i,


gray) increased alongside astrocyte Ca2+ (Fig. 3i, magenta) and astrocyte Ca2+ appeared to peak when neuronal activity began to diminish (Fig. 3i). To investigate this further, we looked at


the average arousal PC around the onset of all astrocyte Ca2+ events. We similarly found that astrocyte Ca2+ events occurred at the peak of arousal-associated neuronal activity (Fig. 3j, top


left), and using the first derivative of the neuronal PC (Fig. 3j, bottom left), we saw astrocyte Ca2+ occurred at a transition point between increasing and decreasing arousal-associated


neuronal activity. This was also true for astrocyte Ca2+ events during stationary periods (Fig. 3j, right). These results indicate that astrocyte activity is positioned to counteract the


effects of arousal on the local neuronal population. These results raised the possibility that astrocyte Ca2+ may respond to changes in local arousal-associated neuronal activity, rather


than arousal or NE per se. To dissect the effects of neuronal activity and arousal on astrocyte Ca2+ we used Random Forest Regression to predict astrocyte Ca2+ (Extended Data Fig. 4). Using


this strategy, we could explain ~85% of the variance in astrocyte Ca2+ fluorescence (Extended Data Fig. 4a, left). Permutation-based feature importance analysis indicated that pupil diameter


was the most important predictor of astrocyte Ca2+, and a substantially better predictor than the next most important factor, local neuronal Ca2+ fluorescence (Extended Data Fig. 4a,


right). These results remained consistent when using the neuronal arousal PC data (Extended Data Fig. 4b). We interpret these results as evidence that astrocytes, while responsive to local


neuronal activity, are sensitive to arousal beyond the influence of nearby neurons. AROUSAL-DRIVEN ASTROCYTE CA2+ IS NOT LOCAL NEURON-DEPENDENT To further investigate how arousal and local


neuronal activity drive arousal-associated astrocyte Ca2+, we expressed hM4Di, an inhibitory Gi-coupled Designer Receptor Exclusively Activated by Designer Drugs (DREADD)30 in neurons, as


well as GCaMP6f in astrocytes to image Ca2+ (Fig. 4a). We found no difference in the average frequency of astrocyte Ca2+ events from baseline following administration of either the hM4Di


agonist CNO or saline, although the overall variability increased (Fig. 4b, resampled distributions from each condition). We also found no difference in astrocyte Ca2+ responses to movement


with either saline or CNO administration (Fig. 4c,d and Supplementary Table 4). There was no difference in astrocyte Ca2+ responses to arousal during stationary periods, except at a high CNO


concentration (5 mg kg−1), where we recorded a potential enhancement of arousal-associated Ca2+ (Fig. 4e,f and Supplementary Table 5). These results indicate that local neuronal activity is


not necessary for astrocyte Ca2+ responses to arousal, and that astrocytes may monitor the state of local circuit activity when responding to arousal. NE TIES ASTROCYTE CA2+ TO CHANGES IN


CORTICAL STATE In Fig. 3, we showed that astrocyte Ca2+ events occur before reductions in arousal-associated neuronal activity. We wondered whether astrocyte Ca2+ was similarly related to


activity changes in the broader cortical circuit. To answer this question, in a subset of mice expressing Ca2+ indicators in neurons (hysn-GCaMP6f) and astrocytes (GFAP-jRGECO1b), we


implanted low-impedance electrodes bilaterally into the visual cortex (Fig. 5a). Using this methodology, we recorded the LFP (Fig. 5b, top), which unlike our spatially restricted imaging


window, reflects the integrated electrical inputs and activity of the visual cortex and surrounding brain regions31. In these LFP recordings, we observed spontaneous transitions between


cortical states dominated by LF power (2–7 Hz; running-evoked 7–10 Hz was excluded) and those dominated by HF (70–100 Hz) power, indicative of synchronous and desynchronized cortical states


respectively (Fig. 5b)1. We noticed that, during transitions to a low-arousal state following movement, astrocyte Ca2+ peaked as LF power increased (Fig. 5c, left) and HF power decreased


(Fig. 5c, right). To investigate this relationship, we cross-correlated astrocyte and neuronal Ca2+ with LFP power, and with the derivative of LFP power. We found that astrocyte


cross-correlations with LFP power were right-shifted from the equivalent neuronal cross-correlations (Fig. 5d,e). When looking at LF power specifically (Fig. 5d, left, magenta), we found


that astrocyte Ca2+ preceded increases in LF power (Fig. 5d, left, magenta). In contrast, neuronal Ca2+ was only significantly positively correlated with LF power with zero lag (Fig. 5d,


left, gray), indicating that LF power and neuronal population activity are coordinated. These findings were confirmed when examining the derivative of LF power. We found that changes in LF


power were maximally correlated with astrocyte activity without any lag (Fig. 5d, right, magenta), while LF power changes preceded neuronal activity (Fig. 5d, right, gray). Our results


demonstrate that, while neuronal Ca2+ is correlated with LF power, astrocyte Ca2+ is correlated with changes in LF power. We found a similar relationship when using HF power, although


inverted about the _y_ axis. HF power preceded both neuronal and astrocyte Ca2+, with neurons maximally negatively correlated with zero time lag (Fig. 5e, left). In addition, both astrocyte


and neuronal Ca2+ were negatively correlated with the derivative of HF power, but for astrocytes this relationship was true both when HF power preceded or had no lag with astrocyte Ca2+


(Fig. 5e, right). These results indicate that, while HF power precedes both neuronal and astrocyte Ca2+, neuronal Ca2+ is inversely related to absolute HF power while astrocyte Ca2+ is


inversely related to changes in HF power. Overall, this analysis demonstrates that neuronal Ca2+ activity reflects absolute LFP power while astrocyte Ca2+ is instead tied to changes in LFP


power. We next asked whether arousal-driven astrocyte Ca2+ was generally tied to changes in LFP power by computing an astrocyte Ca2+ event-triggered spectrogram. We found that astrocyte Ca2+


signaling occurred at the crux of a transition from a HF-dominated cortical state to one dominated by LF power (Fig. 5f). This relationship was also seen in the LFP power of the


contralateral cortex (Fig. 5g), indicating that astrocyte Ca2+ is tied to the transition of neuronal activity from a high- to low-arousal state not just at a local level (Fig. 3j), and at


the level of the nearby cortex (Fig. 5f), but also to bi-hemispheric changes in cortical state. On the basis of our identified changes in arousal and NE as major drivers of spontaneous


changes in astrocyte Ca2+ (Figs. 1 and 2), we hypothesized that NE was necessary for the link between astrocyte Ca2+ and cortical state transitions. In particular, we hypothesized that Adra1


receptors might underlie this relationship due to their importance for astrocyte physiology14,16,19,32. We pharmacologically blocked Adra1 receptors using Prazosin (5 mg kg−1,


intraperitoneal (i.p.)) and found that the relationship between astrocytes and cortical state was reduced (Fig. 5h,i), confirming that NE signaling links astrocyte Ca2+ to cortical state


changes. ENRICHMENT OF ADRA1A MRNA IN VISUAL CORTEX ASTROCYTES We next sought to determine which Adra1 receptors were most likely to underlie the connection between astrocytes and cortical


state. We analyzed a previously published dataset that profiled the ribosome-associated messenger RNA expression of astrocytes in the mouse visual cortex33. We looked at adrenergic receptor


expression in the adult (P120) dataset and confirmed astrocytic expression of most adrenergic receptors, although astrocytes showed little Adra2b, Adrab2 and Adrab3 in this dataset (Extended


Data Fig. 5a, left). When analyzing the astrocytic expression of adrenergic receptors relative to an input control, the relative expression of Adra1a mRNA was highest and greater than the


input control, indicating that Adra1a mRNA may be preferentially enriched in visual cortex astrocytes (Extended Data Fig. 5a, right). We also used spatial transcriptomics to assess the mRNA


expression of Adra1a, Adra1b and Adra2a (Extended Data Fig. 5b). Using LaST map single-molecule in situ hybridization (smFISH)34, we saw striking heterogeneity throughout the brain (Extended


Data Fig. 5b, left). All three receptors showed cortical expression in astrocytes, as delineated by expression of the astrocyte-specific mRNA SlcA3 (GLAST), and in non-astrocytic cell types


(Extended Data Fig. 5b, right). We quantified mRNA spots per astrocyte in the visual cortex for each of these receptors and found higher expression at deep layers of cortex (Extended Data


Fig. 5c). This was particularly true for Adra2a and Adra1b receptors, while Adra1a receptors also showed higher expression in intermediate layers of cortex (Extended Data Fig. 5c), where the


effects of cortical synchrony are particularly important for perception35. ASTROCYTE ADRA1A RECEPTOR SIGNALING SHAPES NEURONAL ACTIVITY On the basis of pharmacological and transcriptomic


data, as well as its activation of astrocytes in other contexts15,16,17,36, we identified Adra1a receptors as a likely connector between astrocytes and cortical state. To test how Adra1a


receptors modulated cortical activity, we injected the Adra1a receptor agonist A61603 (10 μg kg−1, i.p.)—which stimulates astrocytes in acute cortical slices32—while recording cortical


astrocyte and neuron Ca2+ activity (Fig. 6a). We saw robust responses within minutes of A61603 administration (Fig. 6b). Astrocyte Ca2+ was more homogeneous (Fig. 6c) and elevated (Fig. 6d,


left), while neuronal Ca2+ showed a general reduction in baseline Ca2+ (Fig. 6d, right), while exhibiting similar oscillatory activity as astrocytes. To better quantify these neuronal


changes, we took the power spectrum of each neuron and separated the activity into slower (<0.05 Hz, Fig. 6e, left) and faster fluctuations (>0.05 Hz, Fig. 6f, left). We found that


after A61603 administration there was more power in <0.05 Hz fluctuations (Fig. 6e, right) and less power in >0.05 Hz fluctuations (Fig. 6f, right). Our results indicate that A61603


administration, while increasing the coordination and level of astrocyte Ca2+ activity, broadly inhibits and alters the pattern of neuronal activity. To determine how astrocytic Adra1a


receptors specifically affect cortical neuronal activity, we generated a mouse line with LoxP sites flanking _Adra1a_, allowing for Cre-specific deletion of the receptor (Extended Data Fig.


6). We injected an astrocyte-specific Cre-GFP virus into the cortex of Adra1afl/fl mice (or wild-type littermate controls), and performed neuronal Ca2+ imaging while recording movement and


pupillometry (Fig. 6g). In agreement with previous work37, we saw astrocyte-specific Cre expression which colocalized with the astrocytic marker S100β, but not the neuronal marker NeuN


(Extended Data Fig. 7). Overall activity in these mice showed more neuronal Ca2+ events (Fig. 6h), as well as less power in <0.05 Hz Ca2+ fluctuations (Fig. 6i) and more power in >0.05


 Hz Ca2+ fluctuations (Fig. 6j), the inverse of stimulating Adra1a receptors using A61603 (Fig. 6d–f). These results suggest NE signaling through astrocyte Adra1a receptors is a major


pathway for modulating the level and pattern of neuronal activity. To ensure these results were not an artifact of imaging rate, we recorded neuronal activity using resonant galvanometers


and saw the same results (Extended Data Fig. 8). We next determined whether astrocyte Adra1a receptors impacted arousal-related neuronal activity. As before (Fig. 3i), we assessed how


arousal-related neuronal activity changed either with movement (Fig. 6k) or stationary pupil dilation (Fig. 6l). In this dataset, the distribution of durations during movement bouts


(Extended Data Fig. 9a) and stationary pupil dilations (Extended Data Fig. 9b) was wide, and differed between _Adra1a__fl/fl_ mice and wild-type controls. To account for this, we analyzed


only arousal-related neuronal activity during the movement (Extended Data Fig. 9b) or pupil dilation event (Extended Data Fig. 9c), including a ~1 s offset to account for a delayed response


in neuronal activity. In both cases, _Adra1a__fl/fl_ mice displayed enhanced arousal-related neuronal activity (Fig. 6k,l). This increase could not be explained by an overall stronger


neuronal connection to arousal; _Adra1a__fl/fl_ neuronal activity was less correlated with pupil diameter than that in wild-type littermates (Fig. 6m). These results suggest that NE


signaling through astrocyte Adra1a receptors regulates both the magnitude and shape of neuronal responses to arousal. NE SIGNALING VIA ASTROCYTE ADRA1A MODULATES CORTICAL STATE On the basis


of the _Adra1a_-dependent relationship between astrocytes and cortical state, we hypothesized that, in contrast to the desynchronizing effect of NE on the cortex generally11, signaling


through astrocytic Adra1a receptors would lead to cortical synchrony. We again injected the Adra1a receptor agonist A61603 (1 μg kg−1, i.p.) while recording cortical LFP (Fig. 7a). Compared


with saline control, A61603 treatment resulted in high-amplitude LFP fluctuations (Fig. 7b) reflected by increased LF power (Fig. 7c,d). In contrast, we saw no significant difference in HF


power (70–100 Hz, Fig. 7e). These effects show that, contrary to the role of NE more broadly10,11,25, stimulation of Adra1a receptors increases cortical synchrony. However, the manipulation


using A61603 was body-wide due to i.p. injection and affected all Adra1a-expressing cells. On the basis of our Ca2+ imaging results (Fig. 6g–m) in _Adra1a__fl/fl_ mice, we wondered whether


astrocytic Adra1a receptor signaling might modulate cortical state. To test this, we used the same receptor knockout strategy and recorded cortical LFP (Fig. 7f). In _Adra1a__fl/fl_ mice,


the cortical LFP was generally higher amplitude than in controls (Fig. 7g), with higher power across all frequency bands (Fig. 7h, left), and higher total LFP power (Fig. 7h, right). These


results further support the idea that NE signaling to astrocytes modulates overall cortical neuronal activity. We also hypothesized that removing astrocytic Adra1a receptors would effect


NE-related cortical state transitions. We focused on times when mice stopped moving (Fig. 7i, top row), and found _Adra1a__fl/fl_ mice had increased HF power during movement (Fig. 7i, middle


row; Fig. 7j) and less LF power in the _Adra1a__fl/fl_ mice compared with wild-type mice (Fig. 7i, bottom row; Fig. 7k). Taken together, these data show that selectively removing a NE


receptor from astrocytes alters arousal-related cortical state changes, enhancing the desynchronizing effects of arousal and reducing resynchronization afterwards. DISCUSSION Understanding


awake cortical state regulation is crucial for understanding perception, attention and behavior1. Most research examining cortical states has focused on arousal mechanisms—such as release of


NE—that desynchronize the cortex and increase sensitivity to external stimuli6,7,24. However, we found that NE (Fig. 8, green) not only desynchronizes cortical neuronal activity, but also


leads to cortical synchrony by activating astrocytic Adra1a receptors. This model identifies astrocytes as key regulators in the awake cortex, acting as a feedback mechanism for


arousal-associated desynchrony (Fig. 8). ASTROCYTES REGULATE AROUSAL-ASSOCIATED CORTICAL CIRCUITS We found that astrocytes responded more sensitively to arousal (Fig. 1) and NE (Fig. 2) than


previously recognized14,15,16,17. Arousal-associated astrocyte Ca2+ activity occurred at the crux of reductions in arousal-associated neuronal activity (Fig. 3) and bi-hemispheric cortical


state changes (Fig. 5), and was not dependent on local neuronal activity (Fig. 4). These results suggest direct NE signaling to astrocytes acts as a separate neuromodulatory pathway. To


support this, we found that NE signaling through astrocyte Adra1a receptors regulates overall neuronal activity (Fig. 6h–j), the response of neurons specifically to arousal (Fig. 6k–m), and


arousal-associated cortical states (Fig. 7f–k). Notably, we find that astrocytes detect relative changes in arousal, suggesting they act as a feedback mechanism without working against the


arousal system more generally. This role may be particularly useful in the context of heterogeneous cortical NE dynamics. We observed extracellular fluctuations in NE26 on a timescale of


seconds, similar to the reported activity patterns of the underlying locus coeruleus axons28, as well as much slower signaling on the order of tens of seconds to minutes (Fig. 2c). Thus,


change detection may allow astrocytes to ignore the tonic fluctuations of cortical NE and sensitively respond to phasic increases in NE. ASTROCYTE CA2+ IS POISED TO REGULATE NEURONAL


ACTIVITY Of course, astrocytes are not the sole detectors of cortical NE. Neurons, among other cell types12,13, also show strong responses to arousal2,3,7,24 and NE10. Understanding the


relative effects of arousal on neuronal and astrocytic activity is crucial to understanding how these cellular populations contribute to arousal-mediated cortical state changes. Our results


are notable in the context of previous research placing astrocyte activity downstream of neuronal activity, or to driving changes in neuronal activity on long timescales32,38,39. In


contrast, our data show that arousal-associated astrocyte Ca2+ signaling occurs at the crux of the neuronal response to arousal, co-occurring with transitions in arousal-associated neuronal


activity (Fig. 3). This relationship was also seen more broadly, with astrocyte Ca2+ occurring when bi-hemispheric arousal-associated desynchronized electrical activity decreased and


cortical synchrony increased (Fig. 5). Furthermore, we found that NE-specific astrocyte Ca2+ signaling, and its relationship to arousal, was not dependent on the activity of nearby neurons,


suggesting that astrocytes act directly downstream of neuromodulatory signaling to modulate neuronal activity (Fig. 4). These findings support a model in which astrocytes dynamically respond


to NE to modulate neuronal activity on the physiological timescales of arousal. RECEPTOR-SPECIFIC RELATIONSHIP BETWEEN NE AND CORTICAL STATE Our work positions cortical astrocytes as


drivers of neuronal synchrony on multiple scales in the wake state, and suggests new roles for NE in cortical state regulation. In contrast to the generally desynchronizing role of NE11, we


found that specific pharmacological stimulation of the Adra1a receptor reduced cortical neuronal activity (Fig. 6d, right) and altered its pattern (Fig. 6e, f). Adra1a receptor stimulation


also led to cortical synchrony increases without altering HF power (Fig. 7a–d). This relationship was initially hypothesized by early pharmacological work40, but to our knowledge has not


been validated nor widely accepted. Our findings suggest that even within the same family, activation of different NE-receptor subtypes may have profoundly different effects on cortical


state and by extension arousal, attention and behavior, which may help explain disparate effects of adrenergic signaling on perception and cognition41,42. WHAT IS AROUSAL? Here we used pupil


diameter as an external read-out for a complicated set of biological processes that influence neural activity brain-wide23,25,43,44. While we focused on NE, many neuromodulators including


acetylcholine28,45 and serotonin46 vary with arousal and modulate cortical state. Fully describing how neuromodulatory inputs affect astrocyte and neuronal activity will be vital for a


complete description of cortical state regulation. Other internal states, such as motivation, interact with arousal and may involve neuromodulatory systems, but are not fully captured with


the present arousal metrics. Here we were interested in pupil diameter and movement as external readouts of NE-related states, but future work should investigate the contributions of other


internal states, using tools such as facial motion energy29, to further dissect astrocyte function in the context of internal states. While our work establishes a role for astrocytes in


mediating arousal-associated changes in neuronal activity and cortical state, we did not directly link these changes to behavioral outcomes. Future studies should focus on how


arousal-associated astrocyte Ca2+ influences the general perceptual effects of arousal7 and extend these findings to the specific effects of attention1,35,43,47. It will also be important to


examine how sensory stimuli-driven48,49,50 and arousal-driven astrocyte Ca2+ signaling leads to changes in behaviorally relevant neuronal population activity and cortical synchrony. HOW


DOES AROUSAL MODULATE DIFFERENT CELLULAR SUBPOPULATIONS? To expand the impact of our findings, the experiments described here could be extended to dissect the role of specific subpopulations


of neurons and astrocytes, or types of Ca2+ activity in these populations. In this work, we analyzed Ca2+ imaging data as homogeneous cellular populations, in part due to an acquisition


rate (~2 Hz) necessary for imaging astrocyte populations on a wider scale (0.5 mm2). However, there may be differences between the population-level Ca2+ activity we identified and fast Ca2+


responses to arousal. Both astrocytes34,51 and neurons52 can be split into multiple subpopulations, and neuronal subtypes—in particular inhibitory interneuron subtypes—have unique


relationships to arousal and cortical state53. In our work, we used PC analysis to account for heterogeneous neuronal responses to arousal, and we found Adra1a-mediated astrocytic modulation


of neuronal responses to arousal. However, we did not identify any specific effects on neuronal subtypes. On the basis of the overall reduction of neuronal activity with A61603 injection


(Fig. 6d, right), and the overall increase in neuronal activity (Fig. 6h) and LFP power with knockout of astrocytic-Adra1a receptors (Fig. 7h), our work suggests astrocytic modulation of


cortical inhibition is a likely candidate for the downstream circuit mechanisms controlling cortical state, as has been proposed in other contexts36,54. Cortical interneurons have been shown


both to play a critical role in the control of cortical state45,55,56, and to be particularly sensitive to their electrostatic extracellular environment57. Neuromodulator-driven astrocytic


modulation of the extracellular environment58 and inhibitory regulation of nearby neurons18 may act as prime loci of control for cortical circuit activity and state. Within our smFISH


dataset (Extended Data Fig. 5) and in published single-cell data51, cortical astrocytes show variable expression of neuromodulatory receptors, and some astrocytes lack any transcripts for


Adra1a. This suggests molecularly distinct, and potentially functionally distinct, subpopulations of cortical astrocytes with differential sensitivity to arousal-related neuromodulators. It


also suggests that gap junctions, ATP signaling and other mechanisms59,60 that create networks within the astrocyte syncytium may be important for arousal-associated astrocyte activity and


modulation of cortical circuits. Identifying the specific relationships among subpopulations of astrocytes and neurons, and determining the manner and magnitude of their modulation by


arousal, will be important for understanding what constitutes a cortical circuit and how cortical circuit activity is regulated. Furthermore, much like the effects of arousal, these


relationships may be layer35 or cortical area44 specific. Future study of cellular subpopulation-specific effects on cortical state, particularly in additional cortical regions and in


combination with behavioral assessments, will provide a richer appreciation of the cellular mechanisms that regulate arousal-associated cortical state. METHODS ANIMALS All procedures were


carried out in accordance with protocols approved by the University of California, San Francisco Institutional Animal Care and Use Committee. Animals were housed and maintained in a


temperature-controlled environment on a 12 h light–dark cycle, with ad libitum food and water. Male and female mice were used whenever available. All imaging/electrophysiology experiments


were performed at the same time each day. Adult C57BL/6 mice, _Adra1a__fl/fl_ mice or _Adra1a_ wild-type mice aged 1–6 months at time of surgery were used. For experiments involving _Adra1a_


_fl/fl_ mice, the experimenter was blind to animal genotype before surgery, recording and analysis. GENERATION OF ADRA1AFL/FL MICE The Mouse Biology Program at the University of California,


Davis, constructed the mouse. A floxed FLAG-α1A knock-in vector was made using standard methods as follows: The targeting vector contained a 5′ arm of 5.4 kb and a 3′ arm of 5.5 kb. Lox P


sites were placed upstream and downstream of the α1A-AR gene first coding exon. A Kozak sequence and single FLAG tag were upstream, and the neomycin-resistance gene was downstream. The


vector was electroporated into the C57BL/6N ES cell line JM8.F6. The resulting ES cell clones were screened by long-range PCR for loss of the native allele and homologous recombination, and


containing a single copy of the plasmid by LoxP PCR. Two clones passed these screens and had normal chromosome counts. Both ES clones were microinjected into blastocysts, and transferred to


embryonic day 2.5 stage pseudo-pregnant recipients. The resulting chimeras were screened for percent ES cell derived coat color, and those greater than 50% were mated to C57BL/6N females.


Germline heterozygous mice were produced, and mated to MMRRC strain C57BL/6-Tg(CAG-Flpo)1Afst/Mmucd, RRID: MMRRC:036512-UCD, for excision of the Neo selection cassette. Neo-excised mice were


identified via PCR, and mated further to C57BL/6J mice to remove the FLP transgene. Mice were continued in C57BL/6J. Routine PCR genotyping used 5′-gcttcctcaggctcacgtttcc and


3′-gccttagaaatgttcacctgtgc primers upstream and downstream of the LoxP site (Extended Data Fig. 6). These mice are available upon request from the corresponding author. SURGICAL PROCEDURES


AND VIRAL INFECTION Mice were administered dexamethasone (5 mg kg−1, subcutaneous) at least 1 h before surgery, and anesthetized using 1.5% isoflurane (Patterson Veterinary Supply,


78908115). After hair removal and three alternating swabs of 70% ethanol (Thermo Fisher Scientific, 04-355-720) and Betadine (Thermo Fisher Scientific, NC9850318), a custom-made titanium


headplate was attached to the skull using cyanoacrylate glue and C&B Metabond (Parkell, S380). If recording LFP, 0.5 mm burr holes were made bilaterally over the visual cortex, and


bilaterally over the cerebellum for reference, and a ~200-µm-diameter perfluoroalkoxy-coated tungsten wire (A-M Systems, 796500) was implanted -0.2 mm into each hole and secured with


Metabond. For imaging and LFP experiments, a 3 mm craniotomy was made over the right visual cortex and the right visual cortex burr hole was made lateral to the craniotomy. For viral


infection, 400–800 nl total volume of the following viruses were injected alone, or in combination by premixing the solutions before aspiration: AAV5.GfaABC1D.GCaMP6f.SV40 (Addgene,


52925-AAV5), AAV9.hSyn.NE2h (WZ Biosciences, YL003011-AV9), AAV9.GfaABC1D.jRGECO1b (Vigene, custom-ordered), AAV9.Syn.GCaMP6f.WPRE.SV40 (Penn Vector Core, AV-8-PV2822),


AAV2.hSYN.hM4D(Gi).mCherry (Addgene, 50475-AAV2) and AAV5.GFAP(0.7).EGFP.T2A.iCre (Vector Biolabs, VB1131). Injections were made through a glass pipette and UMP3 microsyringe pump (World


Precision Instruments) into one or two locations in the right visual cortex at coordinates centered on +2.5 mm medial/lateral, +0.5 mm anterior/posterior and −0.3 dorsal/ventral from lambda.


After allowing at least 10 min for viral diffusion, the pipette was slowly withdrawn and a glass cranial window implanted using a standard protocol61. For in vivo fiber photometry


recordings, GRABNE2h (AAV9.hSyn.NE2h) and astrocytic jRGECO1b (AAV9.GfaABC1D.jRGECO1b) were expressed via viral vectors in C57Bl/6 mice. A 1-mm-diameter craniotomy was made over the PFC


(+1.7–1.8 mm rostral, +0.5 mm lateral from bregma), and viral vectors were delivered to −2.3 to 2.4 mm ventral. A fiber optic cannula (Mono Fiberoptic Cannula, 400 µm core, 0.66 NA, 2.8 mm


length, Doric Lenses) was then lowered to −2.3 mm ventral and secured in place using dental cement. IMMUNOHISTOCHEMISTRY AND IN SITU HYBRIDIZATION IMMUNOHISTOCHEMISTRY Following in vivo


experiments, mice were overdosed on isoflurane and then perfused transcardially with phosphate-buffered saline (PBS, Sigma-Aldrich P3813) followed by 4% paraformaldehyde in PBS (Santa Cruz


Biotechnology, CAS 30525-89-4). Brains were removed and postfixed overnight in 4% paraformaldehyde, followed by cryoprotection in 30% sucrose in PBS for 2 days at 4 °C. Brains were snap


frozen in dry ice and stored at −80 °C until adhesion onto a sectioning block with Optimal Cutting Temperature Compound (Thermo Fisher Scientific, 23-730-571). Forty-micrometer coronal


sections were taken on a cryostat and stored in cryoprotectant at −20 °C until immunohistochemistry was performed. For immunohistochemistry, free-floating sections spanning the


rostral–caudal axis were selected and washed with 1× PBS for 5 min three times on an orbital shaker, followed by permeabilization with 0.01% PBS-Triton X for 30 min. Sections were then


blocked with 10% NGS (Sigma-Aldrich, S26-100ML) for 1 h. Immediately after, sections were incubated with chicken α-GFP (1:3,000, Abcam, ab13970) and either rabbit α-NeuN (1:1,000, EMD


Millipore, ABN78) or mouse α-NeuN (1:1,000, Millipore Sigma, MAB377) and rabbit α-S100B (1:500, Millipore Sigma, SAB5500172). Sections were then washed with 1x PBS for five minutes three


times on a shaker, followed by secondary incubation with Thermo Fisher Scientific goat α-chicken Alexa Fluor 488 and either goat α-rabbit Alexa Fluor 405 or goat α-mouse Alexa Fluor 405;


goat α-rabbit Alexa Fluor 555 for 2 h at 20 °C on a shaker. Sections were washed again with 1× PBS for 5 min three times, then mounted and cover slipped with Fluoromount-G. For whole section


examples, images were taken using a Keyence BZ-X800 fluorescence microscope to assess viral spread. Then, 2× images were acquired and the images were computationally stitched with Keyence


Analysis Software. For cell counting 60× _z_-stacks were captured on a spinning-disk confocal (Zeiss). Slides were oil-immersed. The Fiji plugin Cell Counter was used to quantify the number


of GFP+, NeuN+ and GFP+/NeuN+ cells to determine colocalization. Each animal had two sections, with each section having six distinct field of views containing 20 _z_-planes. A cell was


considered GFP+ when signal was confined to soma and processes, and GFP+/NeuN+ when cells exhibited merged signals. SINGLE-MOLECULE FLUORESCENT IN SITU HYBRIDIZATION Single-molecule,


fluorescent in situ hybridization data collection was performed using LaST map smFISH as previously described34. Astrocyte cell boundaries were segmented using an ilastik pixel classifier


and a customized watershed segmentation. To preserve processes of astrocyte and not cut them off from the DAPI signals, a pixel classifier was trained by using only large Gaussian filters


(5/10 pixels) during the feature extraction step. As a result, astrocyte processes were detected with fewer splits. Pixel classification carves out only non-background pixels from the image


and does not identify the astrocyte boundaries separating neighboring cells, that is, instance segmentation. To address this problem, we first used CellPose to identify all nuclei from the


image. Subsequently, the centroids of all nuclei were extracted and used as the seeds to generate astrocyte boundaries between adjacent cells using a watershed segmentation. As a result,


astrocytes with touching processes were separated. Finally, as non-cell debris might remain in the segmentation image, we further used an object classification workflow in ilastik to remove


them. All mRNA signals were detected using a Python package called TrackPy using five pixels as diameter and 96 as percentile threshold. These detected spots were then assigned to each


astrocyte that they sat within by using a Python package called shapely. Due to the tissue damage that occurred during the sample preparation step, only seven cortex surface areas from all


sections were eligible for downstream processing to ensure the comparability between tissue sections. For all these regions, both white matter boundaries and the superficial cortex area were


manually annotated. For each cell, the distance to both the white matter boundary (d_WM) and distance to the cortex surface (d_ep) were calculated. The relative cortical depth


(D_relaCortex) was thus defined as: $$D_{{\mathrm{relaCortex}}} = \frac{{d_{{\mathrm{ep}}}}}{{d_{{\mathrm{ep}}} + d_{{\mathrm{WM}}}}}$$ RECORDING SETUP Animals were given at least 1 week


after surgery for recovery and viral expression. They were then habituated on a custom-made circular running wheel over at least 2 days, and for a cumulative time of at least 2.5 h, before


experimental recordings began. After habituation, mice were head-fixed on the wheel and movements were recorded by monitoring deflections of colored tabs on the edge of the wheel using an


optoswitch (Newark, HOA1877-003). PUPILLOMETRY Pupil recordings were made using a Genie near-infrared camera (1stVision, M640) and a telescopic lens (Thorlabs, MVL50TM23), and acquired at 30


 Hz using the MATLAB Image Acquisition toolbox. A small monitor (Amazon, B06XKLNMW3) showing a consistent teal background color (RGB: 0,1,1) was placed by the mouse to allow for observation


of the full range of pupil dynamics in an otherwise dark room. For experiments without 2P illumination, a near-infrared light (Amazon, B00NFNJ7FS) was used to visualize the pupil. 2P IMAGING


2P imaging was performed on a microscope (Bruker) with two tunable Ti:sapphire lasers (MaiTai, SpectraPhysics) and a Nikon 16×, 0.8 numerical aperture water-dipping objective with a 2×


optical zoom (frame rate 1.7 Hz, field of view 412 µm2, resolution 512 × 512 pixels). A 950 nm excitation light with a 515/530 emission filter was used to image green-emitting fluorophores,


and 1,040 nm light with a 605/615 emission filter was used to image red-emitting fluorophores. Recordings lasted from 10 min to 1 h. ELECTROPHYSIOLOGY Visual cortex LFP was recorded at 1 kHz


and subtracted from the ipsilateral cerebellar LFP before 1 kHz amplification (Warner Instruments, DP-304A) and acquired using PrairieView (Bruker) or PackIO62. IN VIVO PHARMACOLOGY


Recordings were taken before and after saline, Prazosin–HCl (5 mg kg−1 Sigma-Aldrich, P7791-50MG), A61603(1 µg kg−1 or 10 µg kg−1, Tocris, 1052), or clozapine N-oxide (CNO, 1 mg kg−1 or 5 mg


 kg−1, Tocris, 4936) were injected intraperitonially while animals remained head-fixed on the wheel, to ensure post-treatment recordings were comparable with baseline measures. FIBER


PHOTOMETRY Dual-color fiber photometry recordings were performed on a Tucker-Davis Technologies RZ10X processor with 405, 465 and 560 nm LEDs. LED drivers were modulated such that light


power was approximately 15 μW for 405 nm and 20 µW for 465 nm and 560 nm wavelengths at the tip of the light path. Animals were recorded in a freely moving arena in which the mouse was able


to move in all directions, after coupling to low-autofluorescence fiberoptic patchcords connected to photosensors through a rotary joint (Doric Lenses). Fluorescence signals were recorded


for 10 min, during which tail lifts were performed every 2 min. For a tail lift stimulation, the experimenter held and lifted the tail of the animal until its hind paws disconnected from the


ground; after that the tail was released. With this experimental paradigm, no pain or harm is caused to the animal. STATISTICS AND REPRODUCIBILITY All data analysis was done in MATLAB


unless otherwise indicated. No statistical methods were used to predetermine sample sizes, but they are similar to previous reports14,28. Box plots are shown with the central mark indicating


the median and the bottom and top edges of the box indicating the 25th and 75th percentiles, respectively. Whiskers extend to the most extreme data point or within 1.5 times the


interquartile range (IQR) from the bottom or top of the box, and all other data are plotted as individual points, as listed in the figure legends. For statistical comparisons, nonparametric


tests were used, or where indicated, normality was assumed but not formally tested, and _t_-tests were used. HB was performed on the basis of a MATLAB implementation


(https://github.com/jenwallace/Hierarchical_bootstrap_Matlab) of the methodology, and used to reduce the statistical error rate of comparisons while retaining statistical power63. All


multiway comparisons were adjusted for using Tukey–Kramer correction. No data were excluded from analyses except for the following (not predetermined): In hSYN-hM4Di experiments, outliers


were excluded across all conditions from small stationary responses to avoid confounding effects from other influences on astrocyte Ca2+, as described in methods. For in vivo pharmacology


experiments, electrical artifacts in band power were excluded before analysis, as described in methods. Samples were allocated into experimental groups by cell-type expression of each


individual fluorescent sensor. Only adult animals (1–6 months of age) were used in experiments, and both males and females were used and randomly selected. For imaging and electrical


recordings of spontaneous activity, blinding was not relevant because cell-type viral expression is evident from expression pattern. For in vivo pharmacology, blinding was not possible


because control recordings were taken before treatment recordings to avoid confounding the treatment effects. For _Adra1a__fl/fl_ mice, the experimenter was blinded to genotype before data


collection and analysis. SPEED CALCULATIONS To compute wheel speed, a detected break in the optoswitch circuit was determined when the absolute value of the derivative of the raw voltage


trace was at least 2 s.d. above the mean. For recordings with very little movement (s.d. <0.1), this threshold generated false positives so a set threshold of 0.1 was used. The number of


breaks in the optoswitch circuit per second was then calculated, and using the circumference and number of evenly spaced colored tabs at the edge of the wheel, the wheel speed was determined


and used for all subsequent analyses using speed. Movement periods were defined by wheel speed ≥10 cm s−1, and movement bouts that were separated by ≤2 s were considered one event. To


ensure that movement-related dynamics were not included in stationary analysis, data were excluded from at least 10 s around identified movement periods. PUPILLOMETRY Following acquisition,


pupil data were processed through a Python function that used contrast detection to identify the edges of the backlit pupil from the sclera and fit an ellipse whose major radius was taken as


the pupil diameter. The diameter was then low-pass filtered to 0.5 Hz and normalized to a range between 0 and 1 to give pupil diameter as percent maximum. The pupil derivate was normalized


to the acquisition rate (30 Hz) to compute pupil phase and to determine the phase of astrocyte Ca2+ events and the cross-correlations with GRABNE. Stationary arousal dilations and


constrictions were identified by the sign of the calculated pupil derivative, and only changes in pupil diameter >10% were used for subsequent analyses. LFP All spectral analysis was done


using Chronux64. Raw LFP data were visually inspected to confirm useable signal was present, and then 60 Hz noise was filtered out and drifting baselines were compensated for using linear


fitting. LFP power for frequency bands was computed using built-in Chronux functions with a time bandwidth of 2.5 and two tapers, no frequency padding and 5 s moving windows. For changes in


LFP band power around arousal or astrocyte Ca2+ events, the median band-limited power was obtained and then normalized to the median band-limited power in the event-triggered time window to


get relative band power. The median power before an event onset versus after was combined for each recording, and for _Adra1a__fl/fl_ mice, the ratio between the two was computed and


compared with _Adra1a_ wild-type mice. For changes in LFP power after A61603 administration, the band-limited power for saline and drug data was calculated, outliers were removed to avoid


contamination by recording artifacts, and then this power was normalized to the band-limited power for the respective baseline recording. For total power in _Adra1a__fl/fl_ and control mice,


no baseline correction was done to avoid skewing the analysis. Spectrum power was calculated by concatenating recordings from all mice of each genotype and computing average or individual


spectra with a time bandwidth of six and eight tapers to increase accuracy. The total power was then computed by summing across all frequency bands. Relative power was computing by dividing


the spectrum from each mouse by its total power, and relative band power was computed by summing the power from each frequency band and dividing by the total power. CA2+ IMAGING Astrocyte


Ca2+ events and fluorescence was extracted using the AQuA software analysis package22. For dual-color imaging with neuronal Ca2+ indicators, particular care was taken to avoid AQuA detection


of neuronal activity; the s.d. of the neuronal channel was taken in FIJI and a mask was created in AQuA to exclude areas of high neuronal activity and soma from analysis. Astrocyte events


were included only if they had an area greater than 10 µm, lasted for at least two frames and had an AQuA _P_ value <0.05. To obtain the average astrocyte Ca2+ fluorescence, the


compensated fluorescence traces that account for spatially overlapping events were taken, normalized to their maximum value and then averaged together. Neuronal Ca2+ events and fluorescence


were extracted from neuropil background semi-automatically using Suite2P65. We identified Ca2+ events by taking identified spikes in the Ca2+ fluorescence data and thresholding them for only


the largest (>3 s.d. over the mean) events. To calculate the average neuronal Ca2+ fluorescence, the trace from each neuron was normalized to its maximum value and averaged together.


MACHINE-LEARNING BASED ANALYSIS OF INPUT CONTRIBUTION TO ASTROCYTE CA2+ As an alternative to assess the contribution of biological inputs on astrocyte Ca2+, data from dual-color Ca2+ imaging


were used to train a machine-learning model to predict average Ca2+ activity. To include LFP data, the spectrogram data from each LFP recording were decomposed using PC analysis based on


the eigenvectors from the ipsilateral recording that accounted for the largest proportion of the variance. The PC1 in this data corresponded to cortical synchrony, with positive weights for


HF and negative weights for low frequencies, matching a previous report but with inverse sign66. LFP PC1 for ipsilateral and contralateral recordings, as well as speed, pupil diameter and


average Ca2+ fluorescence for neurons and astrocytes, was then _z_-scored and resampled to 10 Hz before being concatenated. This dataset was then imported into Python for machine learning


analysis using the SciKit-learn toolbox. For analysis, randomly generated data were added for comparison, and rows without both ipsilateral and contralateral LFP recordings were excluded


from subsequent analysis. Average astrocyte Ca2+ data were used as the target dataset and data were split into training (80%) and testing (20%) before classification using a random forest


regression model. The model was validated using the _R_2 between the predicted average astrocyte Ca2+ fluorescence from the model and the actual average astrocyte Ca2+ data of the test set.


Permutation testing of the predictors was then used to determine their relative contributions to model prediction. GRABNE ANALYSIS In GRABNE imaging data, we observed background fluorescence


fluctuations that we thought might arise from hemodynamic artifacts. To ensure the data reflected the NE signal, hemodynamic artifacts in the data were removed by a custom-designed, data


processing pipeline. The predominant hemodynamic artifact in the data was assumed to reflect fluctuating hemoglobin levels altering brain absorptivity causing an attenuation of light. As


such, the signal from each pixel could be modeled as $$Y_k\left( t \right) = F_k\left( t \right) \cdot e^{ - \mu _k\left( t \right)X} + N\left( t \right) = F_k\left( t \right) \cdot


e^{h_k\left( t \right)} + N\left( t \right)$$ where _k_ is index of pixel, _Y__k_(_t_) and _F__k_(_t_) are respectively the observed curve and the real fluorescence of _k_th pixel,


_μ__k_(_t_) is the absorption coefficient for _k_th pixel, _X_ is the path distance, the term \(e^{h_k\left( t \right)}\) represents the intensity attenuation, and _N_(_t_) is the noise. In


our data, the identified hemodynamic signal across pixels was approximately synchronous but varied in magnitude; thus, the attenuation of one pixel can be represented by another, that is


\(e^{h_j\left( t \right)} = e^{ah_k\left( t \right) + b}\left( \,{j \ne k} \right)\). On the basis the findings above, we designed the following pipeline: * 1. We selected one connected


vascular region with minimal fluorescence in the average projection of the data and calculated an initial vascular reference curve. This region was assumed to have the lowest possibility to


contain any true GRABNE signal. * 2. To avoid compensating for slow changes in the true GRABNE signal, we subtracted the curve of each pixel by a 100-frame moving average. * 3. We applied


linear regression and fit the logarithm of the processed curve to the initial vascular reference curve. The exponential of the fit data was then taken to represent the hemodynamic effect for


each pixel. To account for cases where the initial reference curve was contaminated, we iteratively refined the reference curve before fitting, that is, we calculated the weighted average


of the original curve for all pixels (fitting parameter _a_ in \(e^{ah_k\left( t \right) + b}\) for each pixel is considered as the weight) and subtracted its moving average. * 4. We removed


the hemodynamic artifact (if any) by dividing the raw pixel curve by the exponential of the fitting data, \(F_k\left( t \right) \approx \frac{{Y_k\left( t \right)}}{{e^{h_k(t)}}}\). Next,


only the least (1–25%) hemodynamically affected pixels with the lowest _a_ were taken, excluding the bottom 1%, which often contained artifacts, and these were averaged together and used as


the final GRABNE signal. For spectral analysis, each recording was concatenated together in 10 min segments, padding with its median value if necessary, and then run in Chronux with no


frequency padding, a time bandwidth of 3, five tapers, and passing frequencies above half the window size (3 × 10−3 Hz) and less than the Nyquist frequency (0.9 Hz). To identify phasic


increases in the GRABNE signal, built-in MATLAB functions were used to determine local peaks in the signal and a prominence threshold was used to determine the different magnitudes of GRABNE


increases. EVENT-TRIGGERED AVERAGES All averages were computed by identifying events (for example, movement offset, pupil dilation and so on) and taking data in a symmetric time window


around the events. The data are subsequently plotted as the mean and standard error across all events, except for spectrograms where the median was used. CORRELATIONS For comparisons of


maximum and change in astrocyte Ca2+/pupil/speed after arousal, values were computed for each trace separately and then linearly correlated with _P_ values describing the probability of a


true _R_2 relationship between each two metrics. For correlations between astrocyte and neuronal Ca2+ activity, the average population fluorescence was taken for each and _z_-scored before


cross-correlation. For behavioral state-separated cross-correlations, the same procedure applied, but only _z_-scored data from either moving periods or stationary periods were used. For


correlations within neuronal and astrocyte populations, the pairwise correlation between each cell (neurons) or event (astrocytes) was computed, the symmetric and autocorrelations were


excluded, and the overall mean was taken to obtain a single value indicating the synchrony of Ca2+ dynamics within each cellular population. For cross-correlations between pupil and imaging


data (GRABNE and astrocyte Ca2+), all data were _z_-scored, resampled to either 10 or 30 Hz, padded with nan values if unequal in length, and then cross-correlated. For cross-correlations


between LFP band power and Ca2+ imaging data, all data were _z_-scored, averaged and then resampled to 2 Hz to match the LFP resolution before cross-correlation. HSYN-HM4DI To estimate the


effect of CNO on astrocyte Ca2+, the average Ca2+ event properties and overall event rate for each recording were randomly sampled 104 times and CNO data were subtracted from corresponding


baseline data. This procedure generated the range of treatment effects possible from the sampled data, and a _P_ value was calculated as the proportion of CNO difference from baseline that


was less than the maximum, or greater than the minimum, difference found in saline conditions. For calculating the modulation of astrocyte Ca2+ responses to arousal, the absolute change in


average astrocyte Ca2+ fluorescence after either movement onset or pupil dilation was determined. Outliers during small stationary responses, which might reflect the influence of other


variables on astrocyte Ca2+, were excluded. The magnitude of astrocyte Ca2+ responses to arousal after treatment was then compared with baseline responses. NEURONAL AROUSAL PC ANALYSIS PCA


was done using the built-in MATLAB function on _z_-scored neuronal Ca2+ data. The pupil diameter and PC data were then resampled to an effective rate of 10 Hz, and the Pearson’s correlation


between the pupil diameter and each PC was used to identify the arousal PC for each recording This PC was then normalized to the maximum value before subsequent analysis. For comparisons


between wild-type and _Adra1a__fl/fl_ mice, the response to each movement onset or stationary pupil dilation was normalized to the median value in the window, and then the average arousal PC


value during the event period was taken with a two-frame offset to account for a slight lag in the arousal-associated neuronal response. FIBER PHOTOMETRY Photometry data were detrended


using linear regression to correct bleaching and normalized by _z_-scoring. For startle experiments, recordings were denoised using a FIR filter (cutoff at 2 Hz, transition width 0.5 Hz).


Startle responses were aligned to the onset of the jRGECO signal by fitting a sigmoid to the evoked jRGECO and taking the fourth derivative to identify the onset inflection point. REPORTING


SUMMARY Further information on research design is available in the Nature Portfolio Reporting Summary linked to this article. DATA AVAILABILITY The data presented in this study are publicly


available on Dryad (https://doi.org/10.7272/Q6XK8CS6). CODE AVAILABILITY The code used to generate the findings of this study is publicly available on Zenodo


(https://doi.org/10.5281/zenodo.7098082). CHANGE HISTORY * _ 03 MAY 2023 In the version of this article initially published, the legends for Supplementary Videos 3 and 4 were interchanged


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G. Network homeostasis and state dynamics of neocortical sleep. _Neuron_ 90, 839–852 (2016). Article  CAS  PubMed  PubMed Central  Google Scholar  Download references ACKNOWLEDGEMENTS We


thank G. Chin and S. Yokoyama for technical assistance, K. Roberts and T. Li for help with smFISH data generation, J. Thompson for administrative assistance, and R. Reitman for assistance in


data analysis pipeline construction. We also thank the Poskanzer lab for helpful discussions about the project, and S. Lavrentyeva and E. Kish for comments on the paper. We thank E.


Feinberg and C. Kirst for helpful discussions on the resubmitted paper and experiments, and J. Reimer and C. Smith for discussions related to neuron-astrocyte imaging. This work was funded


by the UCSF Genentech Fellowship (M.E.R.); National Institute of Health R01MH110504 (G.Y.), U19NS123719 (G.Y.), R01NS099254 (K.E.P.), R01MH121446 (K.E.P.) and R01HL31113-27 (P.C.S.);


National Science Foundation 1750931 (G.Y.) and CAREER 1942360 (K.E.P.); Veteran Affairs BX004314 (P.C.S.); and the UCSF Program for Breakthrough Biomedical Research, which is funded in part


by the Sandler Foundation (K.E.P.). The funders had no role in study design, data collection and analysis, decision to publish or preparation of the paper. AUTHOR INFORMATION AUTHORS AND


AFFILIATIONS * Neuroscience Graduate Program, University of California, San Francisco, San Francisco, CA, USA Michael E. Reitman, Drew D. Willoughby & Kira E. Poskanzer * Department of


Biochemistry & Biophysics, University of California, San Francisco, San Francisco, CA, USA Michael E. Reitman, Vincent Tse, Drew D. Willoughby, Alba Peinado & Kira E. Poskanzer *


Bradley Department of Electrical and Computer Engineering, Virginia Polytechnic Institute and State University, Arlington, VA, USA Xuelong Mi & Guoqiang Yu * Wellcome Sanger Institute,


Cambridge, UK Alexander Aivazidis & Omer A. Bayraktar * Department of Medicine and Research Service, San Francisco Veterans Affairs Medical Center and Cardiovascular Research Institute,


University of California, San Francisco, San Francisco, CA, USA Bat-Erdene Myagmar & Paul C. Simpson * Kavli Institute for Fundamental Neuroscience, San Francisco, CA, USA Kira E.


Poskanzer Authors * Michael E. Reitman View author publications You can also search for this author inPubMed Google Scholar * Vincent Tse View author publications You can also search for


this author inPubMed Google Scholar * Xuelong Mi View author publications You can also search for this author inPubMed Google Scholar * Drew D. Willoughby View author publications You can


also search for this author inPubMed Google Scholar * Alba Peinado View author publications You can also search for this author inPubMed Google Scholar * Alexander Aivazidis View author


publications You can also search for this author inPubMed Google Scholar * Bat-Erdene Myagmar View author publications You can also search for this author inPubMed Google Scholar * Paul C.


Simpson View author publications You can also search for this author inPubMed Google Scholar * Omer A. Bayraktar View author publications You can also search for this author inPubMed Google


Scholar * Guoqiang Yu View author publications You can also search for this author inPubMed Google Scholar * Kira E. Poskanzer View author publications You can also search for this author


inPubMed Google Scholar CONTRIBUTIONS M.E.R. and K.E.P. conceptualized and designed the experiments. M.E.R. performed all 2P imaging and physiology experiments, and carried out data analyses


for these experiments. V.T. performed immunostaining experiments and analyses. X.M. and G.Y. worked with M.E.R. and K.E.P. to develop the GRABNE analysis method. D.D.W. performed and


analyzed the fiber photometry experiments. A.P. collaborated on the analysis of 2P imaging and physiology data. A.A. and O.A.B. performed and analyzed smFISH experiments. B.-E.M. and P.C.S.


generated _Adra1a_ floxed mice. M.E.R. and K.E.P wrote the paper with input from other authors. K.E.P. supervised all phases of the project. CORRESPONDING AUTHOR Correspondence to Kira E.


Poskanzer. ETHICS DECLARATIONS COMPETING INTERESTS The authors declare no competing interests. PEER REVIEW PEER REVIEW INFORMATION _Nature Neuroscience_ thanks Inbal Goshen, Nathan Smith and


the other, anonymous reviewer(s) for their contribution to the peer review of this work. This article has been peer reviewed as part of Springer Nature’s Guided Open Access initiative.


ADDITIONAL INFORMATION PUBLISHER’S NOTE Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations. EXTENDED DATA EXTENDED DATA


FIG. 1 DISSECTION OF ASTROCYTE CA2+ AND BEHAVIORAL STATE. (A) Representative 2P mean projection image from one ten-minute recording of _in vivo_ astrocyte GcaMP6f (left, scale bar = 100 µm).


AQuA detected both large (middle) and small (right) astrocyte Ca2+ events within the entire movie, even when they were spatially overlapping. Arrows indicate two pairs of spatially


overlapping events (arrows 1 and 3, and arrows 2 and 4).(B) Traces from the AQuA events shown in (a), with the time period of the AQuA-detected event highlighted in red. (C) Related to Fig.


1c: Individual astrocyte Ca2+ events correlated better with pupil diameter (left, n = 1.2e4 Ca2+ events, One-sided Kruskal-Wallis test) and had a shorter lag with pupil diameter than wheel


speed (right, pupil n = 9.6e3, wheel n = 8.3e3, rank-sum test). (D) Related to Fig. 1d: average pupil diameter during movement (n = 100) and stationary periods (n = 76). (E) Classification


of behavioral state by both pupil diameter and movement. (F) Pupil dilation is smaller (left) and shorter (right, rank-sum tests) during stationary periods (n = 261 dilations, blue) compared


with movement-associated dilations (n = 136 dilations, red, boxplots show median and IQR with whiskers to 1.5 * IQR, two-sided Rank Sum test). (G) Related to Fig. 1l: Left: Movement


duration (n = 104) was related to the maximum wheel speed (top) and pupil diameter (middle), but not to the maximum astrocyte Ca2+ (bottom). Right: the latency to the maximum wheel speed


(top), pupil diameter (middle), and astrocyte Ca2+ (bottom) were strongly linked to movement duration. (H) Heatmap summary of the r2 between the latencies in (g) right, and movement bout


duration. EXTENDED DATA FIG. 2 HEMODYNAMIC CORRECTION OF 2P GRABNE SIGNALS. (A) Left: Average projection of a single GRABNE recording with four regions-of-interest (ROI) in areas with clear


GRABNE fluorescence (black squares, labeled 1–4) and one ROI in a blood vessel (red square, labeled BV). Middle: standard deviation projection. Right: average fluorescence in each ROI before


hemodynamic correction. (B) Left: Estimated hemodynamic signal present in each pixel. Middle: recovered average projection after hemodynamic correction. Note average fluorescence after


hemodynamic correction is broadly similar the uncorrected data in (a) with some blurring due to Gaussian smoothing in preprocessing. Right: average ROI fluorescence after hemodynamic


correction. (C) ROI-free methodology for obtaining GRABNE signal. Left: Following hemodynamic correction, the bottom quartile of pixels with the lowest hemodynamic weights, excluding the


bottom 1% which often had artefactual signals, were kept. Right: These pixels were averaged together to produce the corrected GRABNE signal (bottom) which had substantially less hemodynamic


contamination than the uncorrected field fluorescence (top). (D) Correlation between the corrected GRABNE signal and the uncorrected ROIs in (a) and (b). (E) Left: Correlation between


uncorrected GRABNE fluorescence and pupil diameter. Right: Example traces from the average of pixels that were positively correlated (top), negatively correlated (bottom), or showed little


relationship (middle) with pupil diameter. (F) The corrected GRABNE signal is not similar to the uncorrected GRABNE signal (red dot) but instead reflects the GRABNE signal of binned pixels


(black dots) correlated to pupil diameter (R2 = 0.62, p = 1.55−5, two-sided t-test). EXTENDED DATA FIG. 3 FREELY MOVING FIBER PHOTOMETRY RECORDINGS OF GRABNE AND ASTROCYTE CA2+. (A)


Schematic of fiber photometry recording set-up. (B) A 5-minute example fiber photometry recording of GRABNE signal. (C) GRABNE power spectrum. n = 4 mice, 19 recordings over multiple days,


10–30 minutes/recording. Error lines are ± s.e.m. across all mice.) (D) GRABNE (green) and astrocyte jRGECO1b (magenta) signals evoked by startle responses due to tail lifts (grey arrow


heads). (E) Average startle-response evoked traces for GRABNE and jRGECO, aligned to onset of astrocyte Ca2+. n = 4 mice, 4 tail lifts per mouse. Error is ± s.e.m. across mice. EXTENDED DATA


FIG. 4 ANALYSIS OF CONTRIBUTIONS TO ASTROCYTE CA2+. (A) Left: A Random Forest Regression model was trained (80% of data, 2.3e4 samples) to predict (20% of data, 5.63 samples) average


astrocyte Ca2+ fluorescence accurately (mean r2 = 0.85 ± 4.5e-3 std, n = 10 cross-validations). Right: Relative feature importance based on permutation testing of each predictor. Randomly


generated data was included as a negative control and did not inform model predictions. (B) Same analysis as in (a), using the neuronal arousal PC rather than average neuronal activity.


Random Forest Regression using the neuronal arousal PC showed a similar accuracy to that using mean neuronal fluorescence (mean r2 = 0.87 ± 6.4e-3 std, n = 10 cross-validations). Boxplots


show median and IQR with whiskers to 1.5 * IQR. EXTENDED DATA FIG. 5 CORTICAL ASTROCYTE EXPRESSION OF ADRENERGIC RECEPTORS. (A) Ribosomal-mRNA expression in visual cortex astrocytes of P120


mice from the Farhy-Tselnicker et. al. publicly available dataset. Visual cortex astrocytes show expression of many adrenergic receptors (left) but preferentially express the Adra1a receptor


relative to input control (right). Boxplots show median and IQR with whiskers to 1.5 * IQR (N = 3 mice for astrocyte ribosomal-mRNA and 1 input control). (B) Left: Representative brain


section with Adra1a (green), Adra1b (red), and Adra2a (yellow) mRNA labeled by smFISH using the LaST map pipeline34. SLC1a3 (GLAST) mRNA expression (purple) was used to define the location


of astrocytes. The white square shows a representative ROI used to quantify visual cortex expression. Right: High-magnification image of visual cortex, showing receptor mRNA both within


astrocytes marked by high GLAST mRNA (purple), and outside of astrocytes. (C) Quantification of NE-receptor mRNA expression in visual cortex astrocytes, quantified by relative cortical


depth. Line plots show mean ± std (n = 3 mice, 7 ROIs). EXTENDED DATA FIG. 6 GENERATION OF ADRA1AFL/FL MICE. Top: schematic of the genetic strategy used to generate conditional deletion of


Adra1a. Primers (green arrows) were designed to identify and distinguish between the endogenous and knock-in Adra1a alleles. Bottom: Numbers are in base pairs. Validation of the knock-in


strategy used to generate Adra1afl/fl mice. PCR of Adra1afl/+ mice generates both a 154 base pair band corresponding to the wild type allele and a 235 base pair band corresponding to


successful LoxP knock-in, which is not found in wild-type mice. N = 5 Adra1afl/+ and 4 wild type mice. EXTENDED DATA FIG. 7 ASTROCYTE-SPECIFIC CRE EXPRESSION. (A) Representative average 2 P


image of _in vivo_ neuronal jRGECO1b (gray) and astrocytes expressing Cre-GFP (magenta) (B) Example images show astrocyte-specific Cre-GFP (magenta) expression overlaps with the astrocyte


marker S100β (left, green) but not the neuronal marker NeuN (right, grey), scale bar = 100 µm. (c) Representative mean-projection of a confocal 60x z-stack used for cell counting. Each


animal had two sections with each section having six distinct field-of-views containing 20 z-planes. GFAP(0.7)-Cre-GFP expression (left) was highly astrocytic and the neuronal marker NeuN


(middle) was rarely colocalized (right, scale bars = 50 µm). (D) Cre expression in neurons (grey bars) was low across genotypes (overall = 2.2 ± 0.39 neurons/50 µm3) and no difference was


found between Cre expression in Adra1afl/fl mice and control mice or the cohort as a whole (One-sided Kruskal-Wallis test). (E) Cre-expressing neurons were rare in both wild-type (black,


4.0% ± 0.75%) and Adra1afl/fl mice (green, 4.1% ± 0.65%, two-sided ranked-sum test). (n = 7 Adra1afl/fl and n = 5 wild-type mice for all graphs. Data are presented as mean ± S.E.M.).


EXTENDED DATA FIG. 8 RESONANT GALVO IMAGING (7.5 HZ EFFECTIVE FRAME RATE) CONFIRMS INCREASED NEURONAL ACTIVITY IN ADRA1AFL/FL MICE. (A–C) Histograms show neuronal activity in Adra1afl/fl


(green) and wild-type littermate mice (grey) based on HB. (A) Neuronal Ca2+ event rate was increased in Adra1afl/fl (green, n = 4 mice) compared to wild-type mice (grey, n = 4 mice). (B)


Left: power spectrum of Adra1afl/fl (green) and wild-type (black) Ca2+ activity between 0–0.05 Hz. Right: Total power in 0–0.05 Hz neuronal Ca2+ activity, comparing Adra1afl/fl and wild-type


mice. (C) Same analysis as (b), comparing power in neuronal Ca2+ fluctuations > 0.05 Hz. All p-values from one-sided HB tests. EXTENDED DATA FIG. 9 QUANTIFICATION OF AROUSAL-ASSOCIATED


NEURONAL ACTIVITY. (A) Cumulative distribution plots of the duration of movement bouts (left) and stationary pupil dilations (right) for wild-type (black, n = 400 movement bouts and 1396


pupil dilations) and Adra1afl/fl (green, n = 177 movement bouts and n = 923 pupil dilations) mice. (B) Analysis range (red) used to quantify the normalized arousal PC response to movement in


wild-type (left) and Adra1afl/fl (right) mice. Each row represents one movement event, and the movements from all recordings and mice are concatenated to show the entire dataset (n = 4


wild-type mice and n = 4 Adra1afl/fl mice). (C) Same analysis as in (b), showing stationary pupil dilations in Adra1afl/fl mice compared to wild-type. SUPPLEMENTARY INFORMATION SUPPLEMENTARY


INFORMATION Supplementary Tables 1–5. REPORTING SUMMARY 2P IMAGING OF GRABNE AND ASTROCYTE JRGECO1B. Thirty-minute recording of spontaneous GRABNE (green) and astrocyte jRGECO1b (magenta)


fluctuations in layer 2/3 of visual cortex of an awake mouse. Recording was acquired with a ~410 µm × 410 µm field of view, 10× averaged, and a one-pixel median filter was applied. Video is


played at a 10 Hz frame rate. 2P IMAGING OF NEURONAL GCAMP6F AND ASTROCYTE JRGECO1B. Ten-minute recording of spontaneous neuronal GCaMP6f (gray) and astrocyte jRGECO1b (magenta) fluctuations


in layer 2/3 of the awake cortex. Recording was acquired with a ~410 µm × 410 µm field of view, 10× averaged, and a 0.5-pixel median filter was applied. Video is played at a 10 Hz frame


rate. NEURONAL AND ASTROCYTE CA2+ RESPONSES TO A61603. Neuronal GCaMP6f (gray, left) and astrocyte jRGECO1b (magenta, right) recorded for 30 min at baseline and for 40 min post-injection of


A61603 (10 µg kg−1, i.p.) Labels on the top left indicate pharmacological condition. Recording was acquired with a ~410 µm × 410 µm field of view, 10× averaged, and a 0.5-pixel median filter


was applied. Video is played at a 60 Hz frame rate. 2P _Z_-STACK SHOWING NEURONAL HM4DI AND ASTROCYTE GCAMP6F EXPRESSION IN SAME TISSUE REGION. An ~300 µm _z_-stack of in vivo expression of


neuronal hM4Di-mCherry (gray) and astrocyte jRGECO1b (magenta). The _z_-stack was acquired with a 5 µm step size. A four-frame moving average projection (astrocytes) or s.d. projection


(neurons) was calculated for a display step size of 20 µm per frame. Neuronal data were background-subtracted to aid visualization of soma, and astrocyte data were attenuation-corrected.


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permissions ABOUT THIS ARTICLE CITE THIS ARTICLE Reitman, M.E., Tse, V., Mi, X. _et al._ Norepinephrine links astrocytic activity to regulation of cortical state. _Nat Neurosci_ 26, 579–593


(2023). https://doi.org/10.1038/s41593-023-01284-w Download citation * Received: 04 May 2021 * Accepted: 14 February 2023 * Published: 30 March 2023 * Issue Date: April 2023 * DOI:


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