The V4 RF profile represents a constant-sized, circular sampling of the V1 surface distribution of the visual field (Motter,
2009). Because the visual field representation across the V1 surface is based on the cortical magnification factor (CMF), there is a radial expansion of the receptive field for V4 (and potentially all cortical areas sampling from V1).
Figure 1 illustrates a model V4 RF centered at 4° in the periphery in the lower right visual quadrant; the scaling for the RF is in degrees of visual angle. The RF model was constructed based on a circular sampling of the V1 surface model (Motter,
2009) centered 4° into the periphery and proceeding in 1 mm concentric steps from 1 to 7 mm along the surface. The nested contours represent those steps and generally equate with the sensitivity contours within the RF; sensitivity decreases away from the RF center. The location of highest sensitivity is defined as the RF center even though its location is displaced toward the fovea as a result of the radial asymmetry in sensitivity. The RF maps depicted in the model (
Figure 1) are reasonable matches to actual RF measurements as shown in
Figure 5 and in Motter (
2009).
Figure 1C brings a clear perspective to spatial relationships of stimuli placed at varying distances from the fovea. When a target stimulus is placed at the most sensitive location within the RF, there is an inherent asymmetry in sensitivity to any pair of flanking stimuli placed at equal inward-outward distances from the target stimulus along the radial axis. The inward-outward ratio is roughly 1:2. Three hallmarks of crowding, scaling with eccentricity, a radial inward-outward asymmetry, and a radial-tangential anisotropy of the crowding zone (the area within which crowding is observed) are consistent with the 2D RF as mapped in V4 neurons. The scaling hallmark is matched by the increase of the RF size with eccentricity (
Figure 2A). The inward-outward asymmetry hallmark derives from the observation (
Figure 1C) that for equal target-flanker separations an outward flanker is in a more sensitive part of the RF (and thus more effective) than an inward flanker. The third hallmark of crowding, a radial-tangential anisotropy of the crowding zone, is not a RF property, per se, but can be explained by the inward-outward asymmetry and the common method of plotting the crowding zone. Given that identifying the central target in a dual flanker paradigm requires information from a receptive field centered on the target, then for equally spaced radial flankers the outer flanker will engage the RF at greater distances than the inner flanker (
Figure 1C). In fact the outer radial flanker engages the RF at a greater distance than a flanker in any other direction. In a dual flanker task, the radial extent of crowding is therefore determined by the outer flanker, which leads to plotting a radially elongated crowding zone because the inner and outer limits are both plotted at the same distance from the target. These elongated zones have been reported by Toet and Levi (
1992) and Pelli et al. (
2007) among many others. When a single flanker is used, the resulting crowding zone should appear more like the RF contours in
Figures 1 and
5, and as depicted by Bouma (
1978).