Abstract
In the mammalian cerebral cortex, neural responses are highly variable during spontaneous activity and sensory stimulation. To explain this variability, the cortex of alert animals has been hypothesized to be in an asynchronous high conductance state in which irregular spiking arises from the convergence of large numbers of uncorrelated excitatory and inhibitory inputs onto individual neurons1–4. Signatures of this state are that a neuron’s membrane potential (Vm) hovers just below spike threshold, and its aggregate synaptic input is nearly Gaussian, arising from many uncorrelated inputs1–4. Alternatively, irregular spiking could arise from infrequent correlated input events that elicit large Vm fluctuations5,6. To distinguish these hypotheses, we developed a technique to carry out whole-cell Vm measurements from the cortex of behaving monkeys, focusing on primary visual cortex (V1) of monkeys performing a visual fixation task. Contrary to the predictions of an asynchronous state, mean Vm during fixation was far from threshold (14 mV) and spiking was triggered by occasional large spontaneous fluctuations. Distributions of Vm values were skewed beyond that expected for a range of Gaussian input6,7, but were consistent with synaptic input arising from infrequent correlated events5,6. Furthermore, spontaneous Vm fluctuations were correlated with the surrounding network activity, as reflected in simultaneously recorded nearby local field potential (LFP). Visual stimulation, however, led to responses more consistent with an asynchronous state: mean Vm approached threshold, fluctuations became more Gaussian, and correlations between single neurons and the surrounding network were disrupted. These observations demonstrate that sensory drive can shift a common cortical circuitry from a synchronous to an asynchronous state.
Cortical neurons exhibit variable activity even after efforts are taken to fix temporal variations in sensory stimuli and attentional state8. This ongoing activity affects stimulus encoding and synaptic plasticity9, but its neural basis is not well understood. One hypothesis is that the variable activity in alert animals arises from connections between numerous uncorrelated excitatory and inhibitory inputs1–4. Such a network is consistent with studies of neural architecture10, and exhibits spiking statistics similar to those measured in extracellular studies8. Predictions of this hypothesis2–4,6,7 are that numerous uncorrelated inputs (Fig. 1a, bottom) cause Vm to hover near spike threshold (Fig. 1a, top left) and to exhibit distributions that are near Gaussian or skewed with tails at hyperpolarized potentials (Fig. 1a, top right). In contrast, neurons may receive correlated input5,6 (Fig. 1b, bottom) such that Vm lies far below threshold and exhibits infrequent large excursions (Fig. 1b, top left), forming skewed distributions with tails at depolarized potentials (Fig. 1b, top right). Measurements of Vm from awake, non-behaving cats are suggestive of an asynchronous state11, but are also consistent with correlated input12. Data from behaving rodents in varying attentional states have suggested different pictures13–16, but equivocally, because of the potential contributions of uncontrolled sensory inputs and attentional states to Vm dynamics. Extracellular recordings in drowsy humans have demonstrated correlated spontaneous cortical activity, leaving open the possibility that correlations are absent during alertness17. Accordingly, we carried out the first whole-cell Vm measurements from the cortex of monkeys actively engaged in a visual fixation task, allowing us to examine Vm in single V1 neurons of alert primates while minimizing variability due to sensory stimuli, eye movements, and attentional state.
We obtained intracellular18, whole-cell19,20, current-clamp measurements of Vm from 31 V1 neurons in 3 macaque monkeys while they viewed gratings of different orientations (see Supplementary Section 1 and Supplementary Video). Each trial began when a fixation spot was displayed at the centre of a monitor in front of the monkey. The monkey had to shift gaze to the fixation point and maintain tight fixation for at least 1500 ms to receive a reward. A drifting sinusoidal grating was presented for 1000 ms while the monkey was maintaining strict fixation. We analysed Vm during the fixation period only from trials in which the monkey performed the task successfully. V1 neurons were orientation-selective, and classified as simple or complex (Supplementary Section 2 and Extended Data Fig. 1).
Comparing Vm in blank trials in which no visual stimulus was presented (Fig 2a–c, left) with suprathreshold responses evoked by preferred orientation gratings (Fig. 2a–c, right) shows that blank trial Vm was generally far from spike threshold. There were occasional large depolarizations during blank trials, which manifested in the positive skewness of Vm amplitude histograms, which had longer tails at depolarized potentials, even though traces had had spikes removed (Fig. 2a–c, left, orange histograms; see also Supplementary Section 3 and Extended Data Fig. 2). Across neurons, the median distance between blank trial Vm and spike threshold was 13.9 mV (Fig. 2d). The median skewness of 0.72 (Fig. 2e, f) differs from the near zero or negative skewness expected for a range of Gaussian input (Fig. 1a; see also Supplementary Section 3 and Extended Data Fig. 2c), but is consistent with synaptic input arising from infrequent correlated events (Fig. 1b). These data show that in the absence of visual stimulation, V1 of macaques performing a visual fixation task is not in an asynchronous high conductance state1–4.
By comparison, visual stimulation depolarized neurons (Fig. 2a–c, right; Fig. 3a–c) and decreased the skewness of Vm deviations from the mean (Fig. 3a–c; see also Supplementary Section 3 and Extended Data Fig. 3), an effect significant across the population (Fig. 3d; Wilcoxon sign rank test, p<0.0001; see also Supplementary Section 3 and Extended Data Fig. 4). Together with observed increases in membrane conductance during visual stimulation21,22 (Supplementary Section 4 and Extended Data Fig. 5), these results suggest that visual stimulation shifts the cortical network towards an asynchronous high conductance state1–4.
Visual stimulation also caused significant changes in the power of Vm fluctuations. Membrane potential exhibited greater power at low frequencies than high frequencies during fixation, both before and during visual stimulation. Visual stimulation increased the power of Vm fluctuations from the trial-average (i.e., residuals) at high frequencies (30–50 Hz) but did not cause systematic changes at low frequencies (0.5–4 Hz) (Fig. 3a–c; Fig 3e; Wilcoxon sign rank test, p=0.76 (0.5–4 Hz), p=0.001 (30–50 Hz); see also Supplementary Section 5 and Extended Data Fig. 6). Interestingly, post-stimulus Vm was typically below pre-stimulus levels (Fig. 3f; Wilcoxon sign rank test p<0.0001).
If, as our intracellular recordings suggest, visual stimulation shifts V1 towards an asynchronous state, there should be a concomitant reduction in the correlation between Vm and the surrounding network, as reflected in the simultaneously recorded nearby LFP. This was the case. During fixation with no visual stimulus, deflections indicating spontaneous increases in activity are evident in Vm and LFP (Fig. 4a, left, depolarization for Vm, downward deflections for LFP). These deflections are coincident in both signals (Fig. 4a asterisks); across our population, the zero-lag Vm-LFP cross-correlation was negative during blank trials, reflecting coincident activation of the network and individual neurons, (Fig. 4d, green, median cross-correlation = −0.24, Wilcoxon sign rank test, p<0.01). To determine whether visual stimulation alters this relationship we examined Vm-LFP correlations after trial averages were subtracted (Fig. 4b, c, centre panels). Correlations declined when drifting gratings were presented (Fig. 4b, c, and Fig. 4d; Wilcoxon sign rank test, p<0.01), such that the median cross-correlation was nearer zero (Fig. 4d, lavender; Wilcoxon sign rank test, p=0.91), providing further evidence that visual stimulation drives V1 towards an asynchronous state. The visually-evoked decline in Vm-LFP correlation was apparent for low frequency (0.5–4 Hz), but not high frequency fluctuations (Fig. 4e; Wilcoxon sign rank test, p<0.01 (0.5–4 Hz), p=0.13 (30–50 Hz)); Vm-LFP coherence decreased at low (0.5–4 Hz), but not high frequencies (30–50 Hz) (Fig. 4b, c, right; Fig. 4f; Wilcoxon sign rank test, p<0.05 (0.5–4 Hz), p=0.34 (30–50 Hz); see also Supplementary Sections 5 and Extended Data Fig. 7).
We have shown that in the absence of visual stimulation, V1 in alert behaving primates is not in an asynchronous high conductance state1–4. Rather, spontaneous Vm fluctuations are non-Gaussian and characterized by occasional excursions from rest, consistent with synaptic input arising from infrequent correlated events5,6. In our recordings, sensory stimulation drove V1 towards an asynchronous state, as visually-evoked Vm was closer to spike threshold, exhibited more Gaussian fluctuations, and became less correlated with low-frequency LFP. The visually-evoked reduction in correlation between Vm and LFP is consistent with previously reported decreases in spiking correlations23,24. In an analogous fashion, the correlated activity patterns observed in mouse sensory cortex14 during quiet wakefulness are disrupted by thalamic activation25. (See also Supplementary Sections 6, 7 and Extended Data Fig. 8.) Our records focused on activity in superficial cortical layers; membrane potential characteristics may differ across layers, potentially reflecting laminar specificity in network state26.
How can cortical circuitry support synchronous and asynchronous states? One salient difference between the states was the amount of external input: without visual stimulation thalamic drive to cortex is weak, whereas visual stimulation activates those afferents. We propose that this difference in afferent drive explains the shift in network state. Our proposal unifies observation and theory: a lower input spike rate reduces synaptic input so that Vm lies further from threshold; postsynaptic potentials due to different sources are less likely to overlap in time and appear instead as distinct events. Crucially, theory indicates that a low thalamic spike rate destabilizes the asynchronous state towards low frequency correlations4,27,28, but higher thalamic spike rates drive the network towards an asynchronous state in which correlations weaken4,27,28, as observed in our data. It is clear that external drive alters the cortical state25, but internal factors also play an essential role. In extrastriate cortex, attention causes an increase in overall response that is also accompanied by a decline in the correlation between neurons29,30. Elucidating how these external and internal drives are synthesized will require understanding how V1 interacts with downstream areas.
ONLINE METHODS
All procedures were approved by the University of Texas Institutional Animal Care and Use Committee and conformed to National Institutes of Health standards. Our general experimental procedures in behaving macaque monkeys have been previously described in detail31,32.
Behavioral task and visual stimulus
Three adult male Macaque monkeys (Macaca mulatta) were trained to perform a visual fixation task in which gratings of different orientations were presented. Each trial began when a fixation spot was displayed at the centre of a monitor in front of the monkey. The monkey had to shift gaze to the fixation point and maintain fixation within a small window (< 2° full width) for at least 1500 ms to receive a reward. A drifting sinusoidal grating was presented at a randomized orientation for 1000 ms while the monkey was maintaining strict fixation, thus minimizing variability due to eye movements. (See Supplementary Section 8 and Supplementary Fig. 10 for characteristics of post-fixation saccades.)
Visual stimuli were presented on a gamma-corrected high-end 21 inch color display (Sony Trinitron GDM-F520) at a fixed mean luminance of 30 cd/m2. The display subtended 20.5° × 15.4° at a viewing distance of 108 cm and had a pixel resolution of 1024 × 768, 30-bit color depth, and a refresh rate of 100 Hz. Visual stimuli were generated using a high-end graphics card on a dedicated PC, using custom-designed software. Behavioral measurements and data acquisition were controlled by a PC running a software package for neurophysiological recordings from alert animals (Reflective Computing, St. Louis, MO, USA). Eye movements were measured using an infrared eye-tracking device (Dr. Bouis, Karlsruhe, Germany).
Whole cell recordings
Recording chambers were located on the dorsal portion of V1, with the anterior portion of the chamber reaching close to the lunate sulcus and the border between V1 and V2. We verified the retinotopic organization by voltage-sensitive dye imaging33, and by recording multiunit activity or local field potential with tungsten microelectrodes (Alpha Omega Co, Alpharetta, GA, USA; MicroProbes for Life Sciences, Gaithersburg, MD, USA). The cortex in our cranial windows represents stimuli that are approximately 2.5–5° away from the fovea in the lower quadrant of the contralateral hemifield.
Intracellular records of Vm18,34,35 were obtained with blind in vivo whole cell recordings19–22. The recording chamber was filled with 2–4% agarose in artificial cerebrospinal fluid. Intracellular records were from neurons in the top 1300 μm of V1. As a reference electrode, a silver–silver chloride wire was inserted into the agarose. The potential of the CSF was assumed to be uniform and equal to that of the reference electrode. Pipettes (6–12 MΩ) were pulled from 1.2 mm outer diameter, 0.70 mm inner diameter KG-33 borosilicate glass capillaries (King Precision Glass, Claremont, CA, USA) on a P-2000 micropipette puller (Sutter Instruments, Novato, CA, USA). Patch pipettes were filled with (in mM) 135 K-gluconate, 4 NaCl, 0.5 EGTA, 2 MgATP, 10 phosphocreatine disodium, and 10 HEPES, pH adjusted to 7.3 with KOH (Sigma–Aldrich, St. Louis, MO, USA). Whole cell current-clamp recordings were performed with an Axoclamp 2B Microelectrode Amplifier (Molecular Devices, Sunnyvale, CA, USA). We subtracted 7 mV from all raw membrane potential values to compensate for the liquid junction potential36. (See Supplementary Section 9 and Supplementary Fig. 11 for intrinsic properties of recorded neurons.)
Data Analysis
We analyzed Vm during the fixation period in trials on which the monkey performed the task successfully, and provided mean Vm in the absence of a visual stimulus was less than −50 mV. Vm was detrended by high pass filtering at 0.1 Hz. Data was analyzed with MATLAB (Mathworks, Natick, MA, USA). Shot noise contributions to Vm were assessed by the skewness6,38–40 of Vm distributions. Coherence estimates were performed with Chronux41, a MATLAB library freely available from http://chronux.org/.
Data Analysis for Supplementary Information
The relationship between spike rate and Vm was described with a threshold followed by a power law42–44: R= [θ(Vm−Vr)]α, where θ(x) is the Heaviside step function, Vr is the resting membrane potential, and α is the fitted exponent. Orientation selectivity was assessed with an orientation selectivity index45,46 (vector average = 1−circular variance). Temporal modulation was assessed with the Fourier component of the response with the same temporal frequency as the moving sinusoidal grating visual stimulus divided by the time averaged response47 (F1/F0). Simulations of Hodgkin-Huxley neurons used parameters adapted from Destexhe et al (2001)48 and Pospischil et al (2008)49, and were carried out with Brian50,51. We estimated membrane conductance from voltage responses to hyperpolarizing current pulses of constant amplitude, and a fit of a sum of two exponentials to the voltage response52: V(t) = Iinj[(RM(1−exp(−t/τM))) + (RE(1−exp(−t/τE))) ], where V is the voltage response, t is time, Iinj is injected current, RM is membrane resistance, τM is membrane time constant, RE is electrode resistance, and τE is electrode time constant. Membrane conductance is 1/RM.
Supplementary Material
Acknowledgments
We thank T. Cakic for assistance with this project. We are grateful to J. Hanover and D. Ferster for helpful discussions and comments. A.Y.Y.T., B.S. and N.J.P were supported by grants from the NIH (EY-019288) and The Pew Charitable Trusts; Y.C. and E.S were supported by grants from the NIH (EY-016454 and EY-16752).
Footnotes
Author Contributions
The study was initiated and designed by A.Y.Y.T., E.S. and N.J.P. A.Y.Y.T., Y.C., B.S.,E.S & N.J.P. collected the data. A.Y.Y.T., B.S.,Y.C. and N.J.P. analyzed and modeled the data. A.Y.Y.T., B.S.,Y.C., E.S. and N.J.P. discussed the findings and wrote the paper.
Competing financial interests
The authors declare no competing financial interests.
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