We choose to model the primary visual cortex as a collection of hypercolumns that comprise neurons producing action potentials that are distributed according to Poisson distributions. The firing rate of the neurons depends on the nature of the visual stimulus; conditioned on the stimulus, the neurons are independent and their firing rate does not decay in time. This is an instance of the linear–nonlinear Poisson (LNP) model (Chichilnisky,
2001; Simoncelli, Paninski, Pillow, & Schwartz,
2004), which is commonly used to model neural responses. The anatomy and physiology of these stages of the visual system are well characterized (Hubel & Wiesel,
1962). These mechanisms compute local properties of the image (e.g., color contrast, orientation, spatial frequency, stereoscopic disparity, and motion flow; Felleman & Van Essen,
1991) and communicate these properties to downstream neurons for further processing. Accordingly, we assume that the observer's decision is based on the sequence of action potentials from orientation-selective neurons in V1 (Hubel & Wiesel,
1962). The firing patterns of the neurons are modeled with a Poisson process (Sanger,
1996). While Gaussian firing rate models (Verghese,
2001) have also been used in the past, the Poisson model represents more faithfully the spiking nature of neurons (Sanger,
1996; Beck et al.,
2008; Graf, Kohn, Jazayeri, & Movshon,
2011). In a Poisson process, the number
n of events (i.e., action potentials) that will be observed during 1 s is distributed as
P(
n|
λ) =
λn e–λ /
n!, where
λ is the expected number of events per second (e.g., the firing rate of the neuron).