Motivated by the functional architecture of the primary visual cortex, we analyze solutions to a neural field equation defined on the product space R × S 1 , where the circle S 1 represents the orientation preferences of neurons. We show how standard solutions such as orientation bumps in S 1 and traveling wavefronts in R can destabilize in the presence of this product structure. Using bifurcation theory, we derive amplitude equations describing the spatiotemporal evolution of these instabilities. In the case of destabilization of an orientation bump, we find that synaptic weight kernels representing the patchiness of horizontal cortical connections yield new stable pattern forming solutions. For traveling wavefronts, we find that cross-orientation inhibition induces the formation of a stable propagating orientation bump at the location of the wavefront.
Introduction.Understanding the dynamical mechanisms underlying spatially structured activity states in neural tissue is important for a wide range of neurobiological phenomena, both naturally occurring and pathological. For example, a variety of neurological disorders such as epilepsy and spreading depression are characterized by spatially localized oscillations and waves propagating across the surface of the brain (see Chap. 9 of [10]). Moreover, traveling waves can be induced in vitro by electrically stimulating disinhibited cortical slices [17,39,41,56]. Spatially coherent activity states also arise during the normal functioning of the brain, encoding local properties of visual stimuli [47], representing head direction [50], and maintaining persistent activity states in short-term working memory [27,51]. One of the major challenges in neurobiology is understanding the relationship between spatially structured activity states and the underlying neural circuitry that supports them. This has motivated considerable recent interest in studying reduced continuum neural field models in which the large-scale dynamics of spatially structured networks of neurons is described in terms of nonlinear integrodifferential equations, whose associated integral kernels represent the spatial distribution of neuronal synaptic connections. Such models, which build upon the original work of Wilson and Cowan [54,55] and Amari [1], provide an important example of spatially extended excitable systems with nonlocal interactions. They can exhibit a rich repertoire of spatiotemporal dynamics, including solitary traveling fronts and pulses, stationary pulses and spatially localized oscillations (breathers), spiral waves, and Turing-like