Abstract
Most cortical synapses are local and excitatory. Local recurrent circuits could implement amplification, allowing pattern completion and other computations1,2,3,4. Cortical circuits contain subnetworks that consist of neurons with similar receptive fields and increased connectivity relative to the network average5,6. Cortical neurons that encode different types of information are spatially intermingled and distributed over large brain volumes5,6,7, and this complexity has hindered attempts to probe the function of these subnetworks by perturbing them individually8. Here we use computational modelling, optical recordings and manipulations to probe the function of recurrent coupling in layer 2/3 of the mouse vibrissal somatosensory cortex during active tactile discrimination. A neural circuit model of layer 2/3 revealed that recurrent excitation enhances sensory signals by amplification, but only for subnetworks with increased connectivity. Model networks with high amplification were sensitive to damage: loss of a few members of the subnetwork degraded stimulus encoding. We tested this prediction by mapping neuronal selectivity7 and photoablating9,10 neurons with specific selectivity. Ablation of a small proportion of layer 2/3 neurons (10–20, less than 5% of the total) representing touch markedly reduced responses in the spared touch representation, but not in other representations. Ablations most strongly affected neurons with stimulus responses that were similar to those of the ablated population, which is also consistent with network models. Recurrence among cortical neurons with similar selectivity therefore drives input-specific amplification during behaviour.
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Data availability
Data can be found at CRCNS (http://crcns.org/) at https://doi.org/10.6080/K0Z31WWG.
Code availability
Code for the simulations can be found at https://github.com/jwittenbach/ablation-sim. Code used for data analysis can be found at https://github.com/peronlab/ablation.
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Acknowledgements
We thank S. Druckmann, S. Romani, D. Gutnisky, N. Li, J. Yu, H. Inagaki, N. Sofroniew and M. Economo for comments on the manuscript, A. Hu for histology, and H. Zeng for the Ai162 transgenic mice. Funding was provided by the Howard Hughes Medical Institute. R.P. was supported by the National Institutes of Health (NIH) T32GM007308.
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S.P. and K.S. conceived the project. S.P., R.P. and B.V. performed the experiments, with assistance from H.F.O. J.D.W. performed the modelling, with input from J.F., S.P. and K.S. S.P., R.P., B.V., J.D.W., J.F. and K.S. analysed data and wrote the paper.
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Extended data figures and tables
Extended Data Fig. 1 Effect of ablation in a simulated network with hyper-connectivity (that is, Pconn > 0.4; here, Pconn = 0.44).
Model network responses aligned to input (arrow, bottom). Raster plots show a subset of neurons from an example network. PSTHs show averages across all neurons and networks. Bottom, excitatory neurons within subnetwork. Middle, excitatory neurons outside subnetwork. Top, inhibitory neurons. Left, network response before ablation of 10% of the subnetwork neurons; right, response after ablation.
Extended Data Fig. 2 Multi-photon ablation protocol.
a, Example field of view immediately before (left) and after (right) ablation. Orange arrow denotes target neuron. b, Ablation protocol. Power (orange, top trace) during ablation epochs (100 ms; increased power, orange, top) gradually increased, and the PMT shutter was closed (black bars). During the intervening evaluation epochs, power was lower and constant (orange, top), and the PMT shutter was open. Ablation was terminated when GCaMP fluorescence at the target neuron (green) jumped (orange arrow). c, Success of ablation as a function of neuron depth for all experiments included in this dataset. Individual points give mean success rate for given depth bin; bin size, 25 μm. d, Depth dependence of total energy deposition for successful ablations (successfully ablated cells only: n = 293 cells across 22 sessions, 14 mice; ablations from j250220 and j257218, along with 7 additional ablations from other mice were excluded owing to incomplete logging). Grey dots denote individual ablations. Black dots, means across 25-μm bins. e, As in d, but for peak power needed for ablation (n = 293 cells across 22 sessions, 14 mice).
Extended Data Fig. 3 Multi-photon ablation produces spatially localized effects.
a, Change in calcium event rate (Methods) as a function of minimal distance to an ablated neuron after silent cell ablation. Individual neurons appear as grey points, with dark grey dashed lines showing single mouse averages and the dark black line showing the cross-mouse (n = 8 silent ablation mice) average. Event rates among neurons adjacent to ablated silent cells did not change (event rate before ablation: 0.014 ± 0.008 Hz, grand median ± adjusted MAD; after ablation: 0.014 ± 0.007 Hz; P = 0.055 before versus after ablation, Wilcoxon signed-rank test, paired medians across n = 8 mice; 1,028 neurons across all mice) (Methods). b, Confocal ex vivo image from a mouse perfused 24 h after ablation. Ablation sites are indicated with dashed white circles. Green, GCaMP6s fluorescence; red, mCherry fluorescence; blue, microglial antibody IBA1 fluorescence. c, As in b, but blue shows immunoreactivity for the astrocytic marker GFAP. d, The spatial extent of glial reaction was measured by detecting the fastest intensity decline ridge (dashed white line) in the glial antibody image along lines emanating from the ablation centre at varied angles (Methods). Top, ridge along ablation from b. Bottom left, intensity image in angle-distance space within which the ridge was measured. Bottom right, distribution of reaction radii; all points constitute IBA1 labelling, as no detectable glial reactions were observed with GFAP: 8 out of 10 IBA1-labelled and 0 out of 6 GFAP-labelled ablations retrieved histologically revealed a detectable glial reaction (Methods). These reactions had radii of 11.7 ± 1.7 μm (mean ± s.d.; n = 8 sites). e, Two-photon in vivo images before (left) and after (right) a successful ablation (target, white dotted line). Green, GCaMP6s fluorescence; red, mCherry fluorescence. f, As in e, but after a failure of the ablation protocol to terminate the ablation. Excess energy deposition produced a large lesion (black, centre of image). White arrows denote corresponding points in the two images. Mice (n = 5) with such lesions were excluded from the study.
Extended Data Fig. 4 Effect of ablation on L2/3 model sensory representation increases with the number of ablated neurons.
Ablation effect (change in Rstimulus) as a function of the degree of touch representation degradation (net Rstimulus across ablated neurons). In all cases, we used increased subnetwork connectivity (0.4) (Fig. 1, Methods). The nablated neurons with the highest encoding score were selected for ablation. Grey circles denote individual networks. Black dots denote, median across n = 30 simulated networks for a given number of ablated neurons, indicated in the plot. Beyond nablated > 50, we observed instability, presumably because we did not attempt to restore excitatory-inhibitory balance after ablation; these data were omitted. Correlation of net Rstimulus ablated and ΔRstimulus: R = −0.65, P < 0.01.
Extended Data Fig. 5 Ablation of touch neurons does not produce distance-dependent effects in the whisking representation.
Proximal (15–35 μm to nearest ablated cell) change in Ρwhisking: 0.000 ± 0.192 (grand median ± adjusted MAD); distal (115–135 μm): −0.023 ± 0.186. P value given for Wilcoxon signed-rank test comparing proximal paired to distal (n = 9 mice). Legend as in Fig. 2m.
Extended Data Fig. 6 Behaviour does not account for ablation effects.
a, Pre-touch (dark blue) and post-touch (light blue) distributions of neuron ablation for whisker angle (θ), angle at touch (θ at touch), and net curvature change across all touches (net Δκ at touch) in an example mouse. P values from a Kolmogorov–Smirnov test comparing the distribution of a variable before and after ablation in individual mice. No mice showed a significant (P < 0.05) change in any of the three parameters. b, Fraction of correct trials (left) and number of touches (right) before and after ablation of touch neurons. P values from a Wilcoxon signed-rank test, paired by mouse (n = 9 mice). c, d, As in a and b, but for ablations of silent neurons (n = 8 mice). e, f, As in a and b, but for ablations of whisking neurons (n = 7 mice).
Extended Data Fig. 7 Example effects of ablations of whisking and silent neurons.
a, Example ablation of a whisking neuron. Left, example maps for touch (top, blue) and whisking (bottom, green) cells before ablation. Sphere size corresponds to Rtouch (top) or Rwhisking (bottom) values. Grey dots denote other neurons. These maps exclude the ablated neurons, the position of which is indicated by a faint orange background. Centre, Rtouch (top) and Rwhisking (bottom) values for the ablated population. Right, Rtouch (top) and Rwhisking (bottom) values after ablation, with ablated neurons again excluded. b, As in a, but for ablation of silent neurons.
Extended Data Fig. 8 Simulation of ablation of whisking neurons produces representation degradation in networks with increased, but not equal subnetwork connectivity.
a, Whisking input was simulated by using input with a peak time of 50 ms (bottom), in contrast to 10 ms for touch (top) (Fig. 1). b, Model network responses aligned to input before ablation. Left to right, increasing subnetwork connectivity. Bottom to top, raster plots (each showing a subset of neurons from an example network) and PSTHs (averaged across all neurons and networks) for the three neuronal populations in the model (Fig. 1a, Methods). c, As in b, but after ablation. Thin PSTHs are before ablation. Change in encoding score after ablation: from 0.143 ± 0.024 to 0.104 ± 0.013, grand median ± adjusted MAD. P < 0.001, Wilcoxon signed-rank test paired by network (n = 30 networks).
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Peron, S., Pancholi, R., Voelcker, B. et al. Recurrent interactions in local cortical circuits. Nature 579, 256–259 (2020). https://doi.org/10.1038/s41586-020-2062-x
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DOI: https://doi.org/10.1038/s41586-020-2062-x
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