Figure 3 shows results in two rows for the 0- and 12-dB contrast offset averaged over four normal observers (for fits of individual of each observer see
Supplementary Figs. S2–
S13). We plot the probability of “single flat edge,” “single tilted edge,” and “double edge” responses as a function of disparity. Results shown in the two columns are for two levels of stimulus scale (4 and 32 arc min). Our descriptive model provides an excellent account of these data (solid lines). We provide the fitted parameters in
Table 2, and make comparisons with those parameters to describe the differences within and between our data. In the top row, where the contrast between the two eyes is balanced, three features are evident in both stimulus scales: “Single flat edge” responses dominate at small disparities; “double edge” responses dominate at large disparities, and “single tilted edge” responses (fairly low at all disparities) show a small peak at intermediate disparities, which is approximately balanced between the two eyes. The effects of a contrast offset are seen in the bottom two rows. Introducing a 12-dB contrast difference between the eyes abolishes the fusion response previously seen at small disparities and replaces it with suppression by the eye with higher contrast. It also reduces the degree of diplopia seen at larger disparities, with those responses being replaced by the “one tilted edge” response.
The effect of reducing the mean luminance in one eye using a 2 ND filter (factor of 100) is shown in
Figure 4. The top row is a replotted from
Figure 3, showing the balanced results without an ND filter. The second row shows the effect of putting the filter in front of the nondominant eye. This causes the eye without the ND filter to dominate, particularly at the finer stimulus scale (
EBF ≈ 1). However, there is still a degree of “single flat edge” response at small disparities indicating persisting fusion (fine-scale
pFuse0 = 0.17 versus coarse-scale
pFuse0 = 0.33). We find that the effects of the ND filter are stronger at the finer scale, with the data at the coarse scale showing a smaller effect when the ND filter is introduced.
The remaining two rows show the effect of combining the ND filter with the 12-dB contrast imbalance. At fine scale, increasing the contrast to the eye with ND filter has the effect of reducing the dominance of the other eye (
EBF = 0.52 versus
EBF ≈ 1), increasing fusion at small disparities (
pFuse0 = 0.45 versus
pFuse0 = 0.17) and diplopia at large disparities (
σs = 8.76 versus
σs = 4.99). Increasing the contrast to the eye with the reduced luminance goes some way to balancing out the effects at the fine scale (though fusion is still reduced). At the coarse scale, the 12-dB contrast offset seems to have overcompensated for the effects of the ND filter and introduced an imbalance in the opposite direction. From these results it seems that the effect of the luminance imbalance is scale dependent, and consequently the contrast imbalance necessary to counteract that effect is also scale dependent. In the bottom row of
Figure 4, we show that reducing the contrast of the stimulus seen by the eye with the ND filter results in near-complete suppression of that eye.
Results from amblyopes are presented in
Figure 5. There is suppression of the amblyopic eye evident at all disparities (top row). One of the most remarkable results is that at the coarse scale with no contrast offset there is a dominant “single flat edge” response at small disparities, indicating fusion (
pFuse0 = 0.75). This does not occur at the fine scale (
pFuse0 = 0.18), consistent with the known scale dependence of the amblyopic deficit, where higher spatial frequencies tend to show poorer sensitivity. There is also evidence of diplopia at large disparities for the coarse scale, indicating a reduced suppression range compared to the fine scale (
σs = 9.02 at coarse scale versus
σs = 48.07 at fine scale). When the contrast balance is shifted to favor the amblyopic eye by 12 dB, we also see a difference between the two scales. At the fine scale we observe a reduction in suppression and an increase in fusion. At the large scale, the increased contrast to the amblyopic eye results in a reversal of suppression of the fellow fixing eye by the amblyopic eye, similar to what we saw in the ND results (
Fig. 4). Apart from this reversed suppression, the relationship between fusion and diplopia at this large scale was similar to that found in normal observers and quite different from the anomalous interactions seen at the fine stimulus scale. When the contrast is reduced in the amblyopic eye (bottom row) there is near-complete suppression of the amblyopic eye.
Results from control subjects with ND filters in front of one eye and from amblyopes can be compared using
Figures 4 and
5. There we see a different relationship between suppression and disparity and a reduced degree of diplopia in the amblyopic participants. For the coarse-scale stimulus, suppression at large disparities in the ND filter case is weaker compared to the amblyopic data. Complementary changes are observed for the diplopia. At the coarse stimulus scale, amblyopes show stronger fusion at small disparities and weaker diplopia at larger disparities than exhibited by the ND simulation (amblyopes
pFuse0 = 0.75 versus controls with ND
pFuse0 = 0.33). Although, at the fine stimulus scale, the ND filter does a good job in simulating the amblyopic responses in terms of reducing fusional responses at small disparities (amblyopes
pFuse0 = 0.18 versus controls with ND
pFuse0 = 0.17), amblyopic participants still show larger suppression at larger disparities (amblyopes
σs = 48.42 versus controls with ND
σs = 8.76).