Figure 4 shows variations in global field power as a function of time for both contrast conditions and for all orientation differences separately and graphs of mean field strength as a function of orientation difference in the two component windows for both high- and low-contrast gratings.
The repeated-measures ANOVA for the P100 time window (90 to 110 ms) showed that the field strength for high-contrast stimuli was larger than for low-contrast stimuli, F(1, 13) = 36.06, p < 0.001, η = 0.76. There was also a significant main effect of orientation difference, F(5, 65) = 6.86, p = 0.004, η = 0.35, but no significant interaction of these two, F(5, 65) = 1.06, p = 0.38, η = 0.08. Mean field strength followed a U-shaped function with increasing orientation differences between the dichoptically presented gratings, F(1, 13) = 13.74, p < 0.003, η = 0.51. Excluding the 0° orientation difference yielded the same pattern of results with main effects of contrast condition, F(1, 13) = 31.05, p < 0.001, η = 0.71, and orientation difference, F(4, 52) = 5.52, p = 0.007, η = 0.30, but no significant interaction of these two, F(4, 52) = 1.43, p = 0.25, η = 0.10; a significant quadratic trend for orientation differences, F(4, 52) = 14.80, p = 0.002, η = 0.53, but also a significant linear trend for orientation differences, F(4, 52) = 6.33, p = 0.03, η = 0.38.
The repeated-measures ANOVA for the N170 time window (160 to 180 ms) showed only that the field strength for high-contrast stimuli was larger than for low-contrast stimuli, F(1, 13) = 8.18, p = 0.01, η = 0.39. Neither orientation difference, F(5, 65) = 3.05, p = 0.08, η = 0.19, nor the interaction of contrast condition and orientation difference, F(5, 65) = 1.34, p = 0.28, η = 0.09, was significant. Excluding the 0° orientation difference from analysis preserved the main effect of contrast condition, F(1, 13) = 9.37, p < 0.01, η = 0.42, but also yielded a significant effect of orientation difference, F(4, 52) = 3.75, p = 0.02, η = 0.22. For orientation differences larger than 0°, field strength increased as a function of orientation difference as confirmed by a significant linear trend: F(1, 13) = 13.45, p = 0.003, η = 0.50. The interaction of contrast condition and orientation difference remained nonsignificant, F(4, 52) = 1.33, p = 0.28, η = 0.09.
The global field power results in both the P100 and the N170 time windows are consistent with options a.2 (dependency on the degree of orientation difference) and b.1 (general effect of stimulus contrast independent of orientation difference).