How MT cells analyze the motion of visual patterns Nicole C Rust1, 2, 4, Valerio Mante2, 3, 4, Eero P Simoncelli1, 2, 5 & J Anthony Movshon2, 5 Neurons.

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How MT cells analyze the motion of visual patterns Nicole C Rust1, 2, 4, Valerio Mante2, 3, 4, Eero P Simoncelli1, 2, 5 & J Anthony Movshon2, 5 Neurons in area MT (V5) are selective for the direction of visual motion. In addition, many are selective for the motion of complex patterns independent of the orientation of their components, a behavior not seen in earlier visual areas. We show that the responses of MT cells can be captured by a linear-nonlinear model that operates not on the visual stimulus, but on the afferent responses of a population of nonlinear V1 cells. We fit this cascade model to responses of individual MT neurons and show that it robustly predicts the separately measured responses to gratings and plaids. The model captures the full range of pattern motion selectivity found in MT. Cells that signal pattern motion are distinguished by having convergent excitatory input from V1 cells with a wide range of preferred directions, strong motion opponent suppression and a tuned normalization that may reflect suppressive input from the surround of V1 cells.

Vision's Grand Theorist

Stimulus Space

Component and Pattern Predictions Grating Tuning Curve

Figure 2. Quantification of neuronal responses to plaids. We compared each cell's response to idealized component and pattern predictions (Methods). Briefly, the plaid response is quantified by computing the partial correlation between the actual response of the cell and the component and pattern predictions and taking its Z-score, Z p and Z c. Component predictions are constructed by taking the linear superposition of two half-contrast grating tuning curves shifted by an amount corresponding to the plaid angle and subtracting the baseline response. For all plaid angles, the pattern prediction is the half- contrast grating tuning curve. For most cells (n = 39 of 50), Z p and Z c were computed as the mean Z p and Z c for 60°, 90°, 120° and 150° plaids. For the remaining cells, Z p and Z c are computed based on the responses to gratings and 120° plaids. (a) Z p plotted against Z c for 50 cells. Data for the five cells used as examples in subsequent figures are drawn in gray. (b) The distribution of the difference between Z p and Z c (hereafter the pattern index). The center bin of the histogram includes all cells classified as "unclassed"; cells with larger values are classified as pattern direction selective and cells with smaller values as component direction selective.

Figure 5. Comparison of the pattern index observed and predicted by the cascade model. The diagonal indicates identity. Data from the five example cells from Figure 4 are drawn in gray. We computed predicted pattern indices by simulating the same number of trials acquired during data collection with a Poisson spiking mechanism. Error bars for the actual pattern indices were computed by bootstrap resampling of the data (Methods). Error bars for the predicted pattern indices were computed by bootstrap resampling of the responses to hyperplaids, refitting the data for each sample and computing the pattern index arising from the resulting model (Methods). Error bars indicate one s.d. of the bootstrap distributions.

Figure 7. Relationship between the recovered cascade model parameters and pattern index. (a) The V1 direction tuning curve bandwidth, before normalization. The break in the axis indicates the model V1 cells whose tuning bandwidths are narrower than the resolution tested by these experiments and thus unconstrained by the fit. (b) Strength of the untuned normalization signal, measured by the fit weight 1 (Methods). (c) Strength of the tuned normalization signal, measured by the fit weight 2 (Methods). (d) The fraction of robustly excitatory weights in the recovered MT linear weighting function (those that exceeded 20% of the peak recovered weight). (e) The fraction of robustly inhibitory weights in the recovered MT linear weighting function (those whose magnitude exceeded 20% of the peak recovered weight).