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. 2020 Feb 19;9:e52757. doi: 10.7554/eLife.52757

Figure 3. Patterned perturbation of inhibition based on receptive field similarity is necessary to reveal specific inhibitory stabilization.

(A) Sample neuronal RFs for excitatory (magenta) and inhibitory (blue) neurons and schematics of connectivity between neuronal pairs. (B) Upper: Distribution of RF similarity of all neuronal pairs in the network, as quantified by pairwise correlations of RFs. Lower: Weights of connections between neurons as a function of their RF similarity. (C1) Activity of excitatory and inhibitory neurons in response to patterned perturbation along the 1D dimension of orientation (similar to Figure 2A). (C2) The average activity of neurons during baseline and perturbed states, along with the profile of inhibitory perturbation, as a function of the preferred orientation of neurons (similar to Figure 2B). (D1,D2) Similar to (C1,C2) for patterned perturbation along RF similarity (see Materials and methods). The average activity of neurons in (D2) is plotted against the RF similarity of respective neurons to a reference inhibitory cell. (E) Response change of individual inhibitory neurons as a result of perturbation versus their respective input perturbations, along with the best fitted regression line (red), similar to (C). Patterned perturbation along the 1d feature of orientation does not reveal a negative slope, although it yields a nonspecific paradoxical effect (average increase of inhibition as a result of negative perturbations). (F) Patterned perturbation along RF similarity (with regard to a reference cell) shows the specific paradoxical effect (negative slope). (G) Same pattern of perturbation as in (F) but randomized over inhibitory neurons, does not lead to a specific paradoxical effect (lack of negative slope).

Figure 3.

Figure 3—figure supplement 1. Spectral analysis of specific perturbations.

Figure 3—figure supplement 1.

(A) Connectivity matrix of the excitatory subpopulation (E-to-E) in a network with feature-specific connectivity based on a one-dimensional feature (preferred orientation, PO), as in Figure 2. (B) Connectivity matrix of excitatory neurons based on RF similarity (similar to networks in Figure 3). Neurons are sorted according to their preferred orientations (PO) in both (A) and (B). (C) Spectrum of weight matrix in (B), when specific connectivity is only preserved within excitatory (EE) subnetwork. Connectivity between other connection subtypes (E-to-I, I-to-E, and I-to-I) is replaced with the mean value of the respective subpopulation. The eigenvalue marked in red thus reveals the most unstable eigenmode resulting from specific E-to-E connectivity. (D) Structure of the first specific eigenmode of E-to-E (i.e., the eigenvector corresponding to the eigenvalue marked in red in (C)) versus different features of excitatory neurons: their preferred orientation (Pref. orient.) in left and RF similarity of neurons to a reference neuron in the network on right. Correlation coefficient (CC) between the specific eigenvector and neuronal features are indicated in red in each case. Red lines show the best fitted regression line to the data. (E) Distribution of the absolute value of the correlation coefficient (|CC|) between the specific eigenvector and the vector of RF similarity of neurons to different excitatory neurons in the network. (F,G) Similar to (D,E) for another specific eigenvector (the third unstable eigenvalue marked in blue in (C)).