Averages were checked for each subject individually in terms of data quality, focusing on a clearly distinguishable C1, based on the typical polarity reversal for UVF versus LVF, consistent timing, and expected topography. For all 31 subjects, a clear C1 was detected for all stimulus densities in both the LVF and UVF. Twenty-one subjects showed a canonical, central parieto-occipital C1 topography. Grand-averaged data indicated a C1 maximum at electrode POz in all six conditions, independent of whether all subjects or only those with a canonical C1 topography were included. In the LVF, C1 peaked at 80 ms for stimuli of LD, with an amplitude of 5.56 µV; at 90 ms for stimuli of MD (5.52 µV); and at 94 ms for stimuli of HD (4.61 µV). In the UVF, C1 reached its maximum at 86 ms for LD (−2.91 µV); at 96 ms for MD (−4.58 µV); and at 100 ms for HD stimuli (−4.48 µV).
Figure 2 shows ERP waveshapes based on maximum C1 electrodes selected per participant and condition, as these form the basis of our primary analyses (see Data recording and analyses).
The latency values described earlier suggest substantial delays for higher stimulus densities, in accordance with known differences between magno- and parvocellular pathways conveying low and high spatial frequency information, respectively (
Foxe & Simpson, 2002;
Vuilleumier et al., 2003). Indeed, a 2 × 3 repeated-measures analysis of variance (ANOVA) on latency values with Location and Stimulus Density as within-subject factors showed that higher stimulus densities were associated with later C1 peaks [main effect of Stimulus Density: LD, 83 ± 1 ms; MD, 94 ± 1 ms; HD, 97 ± 1 ms;
F(2, 60) = 156.47,
p < 0.001]. In addition, longer delays were seen in the UVF compared with the LVF [main effect Location: LVF, 88 ± 1 ms; UVF, 95 ± 1 ms;
F(1, 30) = 36.49,
p < 0.001]. Finally, we observed a significant interaction between Location and Stimulus Density,
F(2, 60) = 3.23,
p = 0.046. Follow-up
t-tests indicated that this was due to an only marginally significant difference between UVF and LVF for LD stimuli (
p = 0.087), whereas this difference was highly significant for MD and HD stimuli (both
p < 0.001). The same analysis calculated only for subjects with a canonical C1 topography (
n = 21), based on a pool of four electrodes, yielded equivalent main effects [Location:
F(1, 20) = 22.00,
p < 0.001; Stimulus Density:
F(2, 40) = 147.7511,
p < 0.001]. However, the Location × Stimulus Density interaction was only marginally significant in this case,
F(2, 40) = 3.22,
p = 0.05.
Turning to amplitude values, a 2 × 3 repeated-measures ANOVA with Location and Stimulus Density as within-subject factors indicated stronger C1 responses following stimuli presented to the LVF [main effect Location: LVF, 6.59 ± 0.40 µV; UVF, 4.95 ± 0.44 µV;
F(1, 30) = 14.15,
p < 0.001; note that UVF amplitude values were inverted, see Data recording and analyses]. Results also showed that C1 was maximal in response to MD stimuli [main effect Stimulus Density: LD, 5.32 ± 0.35 µV; MD, 6.15 ± 0.41 µV; HD, 5.84 ± 0.44 µV;
F(2, 60) = 4.02,
p = 0.023]. Importantly, UVF and LVF response profiles differed from each other, as indicated by a significant Location × Stimulus Density interaction,
F(2, 60) = 11.02,
p < 0.001. Follow-up
t-tests between visual field locations for each stimulus density revealed significantly higher C1 amplitudes in the LVF for LD (
p < 0.001) and MD stimuli (
p = 0.010). No such difference was observed for HD stimuli (
p = 0.441;
cf.
Figure 3).
A follow-up ANOVA restricted to the UVF indicated significant differences in C1 amplitudes between stimulus densities [main effect Stimulus Density: LD, −3.84 ± 0.36 µV; MD, −5.40 ± 0.55 µV; HD, −5.59 ± 0.57 µV; F(2, 60) = 10.85, p < 0.001]. Post hoc t-tests indicated lower amplitudes for LD stimuli compared with both MD and HD (LD vs. MD, p = 0.001; LD vs. HD, p < 0.001), in the absence of differences between MD and HD stimuli (p = 0.64). In contrast, in the LVF, there was only a marginally significant effect of Stimulus Density on C1 responses [LD, 6.79 ± 0.44 µV; MD, 6.89 ± 0.41 µV; HD, 6.08 ± 0.50 µV; F(2, 60) = 2.70, ε = 0.68, p = 0.098]. Post hoc t-tests indicated that this was due to higher C1 amplitudes for MD compared with HD stimuli (p = 0.003), in the absence of differences between LD and MD (p = 0.80), or between LD and HD stimuli (p = 0.15).
To quantify the similarity between UVF and LVF C1 responses following HD stimuli, we conducted a Bayesian ANOVA with Location and Stimulus Density as within-subject factors, using standard priors as implemented in JASP 0.10.2. Unsurprisingly, the results were largely analogous to the classical ANOVA reported earlier, with the full model including both main effects and their interaction almost 10 times more likely than the next-best model including only Location. Analysis of individual effects indicated definite evidence for inclusion of the Location factor (Bayes Factor [BF]
incl >500,000), moderate evidence for inclusion of Stimulus Density (BF
incl = 6.87), and strong evidence for inclusion of the Location × Stimulus Density interaction (BF
incl = 24.46). Follow-up Bayesian paired
t-tests also confirmed the results of the classic
t-tests reported earlier, with definite evidence for differences between UVF and LVF for both LD and MD stimuli (both BF
10 >100,000 for standard, wide, and ultrawide Cauchy priors). Importantly, the Bayesian approach allows us to quantify the probability of there being no difference between UVF and LVF C1 responses following HD stimuli. Results showed moderate evidence in favor of H
0, with BF
01 = 3.94. This result remained stable across different prior widths (
Figure 4).
Taken together, the results described earlier indicate important visual field anisotropies during initial processing of high-contrast textures. A potential caveat relates to the overlap between C1 and later, extrastriate components, particularly P1 (
Clark et al., 1995;
Slotnick, 2018). The most problematic condition is usually for LVF stimuli, as the positive-going C1 may be contaminated by the early phase of the P1. In our data, we actually observe a negative component following the positive C1 after LVF stimulation. As shown in
Figure 5, and in line with previous studies using similar stimuli (
Clark et al., 1995;
Pourtois et al., 2008;
Rauss et al., 2009), this component is characterized by a circumscribed, central, parieto-occipital negativity, reminiscent of what
Clark et al. (1995) termed the N90op. As detailed in the Discussion, such a polarity inversion for putatively extrastriate visual evoked potential (VEP) components is likely related to both the extent and eccentricity of the stimuli employed.
To address whether overlaps between C1 and the subsequent P1 or N90op components might have confounded the results reported earlier, we performed a repeated-measures ANOVA with factors Location and Stimulus Density, based on mean amplitudes, calculated over 20 ms time-windows around the grand-average peak latency, separately for each component and each stimulus density (UVF/P1: LD, 130–150 ms; MD, 134–154 ms; HD, 140–160 ms; LVF/N90op: LD, 118–138 ms, MD, 126–146 ms; HD, 128–148 ms). We again used absolute amplitudes (i.e., N90op values were inverted) to allow for easier interpretation of the Location factor. Results indicated differential response profiles in upper and lower visual hemifields [Location × Stimulus Density, F(2, 60) = 24.96, p < 0.001], in the context of globally higher responses in the LVF [main effect Location, F(1, 30) = 10.61, p = 0.003] and overall differences between stimuli [main effect Stimulus Density, F(2, 60) = 10.62, ε = 0.802, p < 0.001]. Importantly, the nature of this interaction was different from that observed for C1: follow-up t-tests indicated higher amplitudes in the LVF compared with the UVF for all stimulus densities (LD, p < 0.001; MD, p = 0.034; HD, p = 0.035, one-sided); and separate follow-up ANOVAs showed that the different stimuli elicited differential responses only in the LVF, F(2, 60) = 38.80, ε = 0.815, p < 0.001; UVF, F(2, 60) = 2.23, ε = 0.848, p = 0.126. Post hoc tests further indicated reduced LVF responses with increasing stimulus density (all pairwise p ≤ 0.008). Taken together, the P1 following UVF stimulation appears statistically flat, whereas the preceding C1 increases and then plateaus with increasing stimulus density. Conversely, the LVF N90op displays a steady decline across increasing stimulus densities, whereas its preceding C1 shows only moderate evidence for a decline at the highest density tested. Given these results, it appears unlikely that differences in the ascending phase of P1 and N90op would explain the differences observed for the preceding C1.