Crossed and uncrossed relative disparity thresholds measured in Experiment 1 are presented in
Figure 2. The gray dots show thresholds from subjects who were not selected for further testing. The square symbols are used for subjects who were further tested in subsequent experiments. Thresholds ranged from 24 to 275 arcsec. Overall, data appear to lie along the diagonal. This indicates a rough agreement between subjects’ crossed and uncrossed thresholds. To further explore this relationship, we performed a Pearson correlation analysis in SciPy (
E. Jones, Oliphant, & Peterson, 2001). Thresholds for the two relative disparity directions were significantly correlated (R = 0.79,
p < 0.001). Most of the points in
Figure 2 lie
above the unity line. This shows a tendency for uncrossed thresholds to be higher than those for crossed disparity. We tested for a mean difference using a
t-test (SciPy) and found it to be significant: t(52), –5.14,
p < 0.001. The geometric mean was 73 arcsec for uncrossed thresholds and 58 arcsec for crossed thresholds. We performed a further analysis on the separate data from the two task repetitions for each subject. From this we found there to be a good test-retest reliability (R = 0.76).
The noise-masking functions obtained in Experiment 2 are presented in
Figure 3. The results from each subject are shown in separate panels. Thresholds are plotted separately for relative crossed and uncrossed disparity. A pair of thresholds are plotted at each external noise standard deviation. Performance for the two directions of disparity without noise (leftmost data point in each plot) were compared using a likelihood ratio test. The results of this test are presented in Table S1 of the
Supplementary material. Subjects 10, 12, 14, 28, 32, and 35 had significant threshold differences for detecting relative crossed versus uncrossed disparity (without external noise). As the external noise level increases, the classic noise masking behavior can be seen. With low levels of external noise, thresholds were constant. Beyond some critical value, however, thresholds increase linearly with external noise standard deviation. Thresholds were fit with the linear amplifier model. Most subjects who showed significant differences without external noise have fitted curves that are vertical translations of each other. This suggests that threshold differences are due to differences in the efficiency of processing for the two directions. There was also evidence, however, of differences in the transition point between the flat and sloped regions of the two curves. This indicates differences in equivalent internal noise.
We performed a series of analyses on the two parameters obtained from the linear amplifier model fits. We found no significant correlation between the equivalent internal noise and efficiency parameters across our 18 subjects. The R
2 scores were 2% for the uncrossed disparity data (
p = 0.622), and 13% for the uncrossed disparity data (
p = 0.150). This suggests that the two parameters do not reflect a single underlying property that varies across our subjects. The noise-masking measurements allow us to ask whether either of the two model parameters are responsible for a larger part of the individual differences in disparity threshold. We analyzed the relationship between the relative disparity thresholds and the fitted model parameters (
Figure 4). We took the thresholds from Experiment 1 and the linear amplifier model parameters from Experiment 2. This meant that the measurement errors affecting the
x- and
y-axes were independent. We used this analysis to investigate how the individual differences in stereo measured in Experiment 1 depend on the factors accounted for by the two model parameters. We performed a separate analysis for sensitivity to crossed (
Figures 4A and B) and uncrossed (
Figure 4C and D) relative disparity. Higher thresholds were associated with increased equivalent internal noise (
Figures 4A and C) and reduced processing efficiency (
Figures 4B and D). For each disparity direction we performed a multiple linear regression (using the ordinary least squares function from the statsmodels Python package;
Seabold & Perktold, 2010). The regression predicted each subject's thresholds from Experiment 1 using the internal noise and efficiency parameters obtained from Experiment 2. The detailed results are presented in the
Supplementary material. For both the crossed and uncrossed disparity results we found that subject-by-subject variation in both equivalent internal noise and processing efficiency contributed to the individual differences. The two parameters explained 73% of the variance for crossed disparity. For uncrossed disparity they explained 79% of the variance. For crossed disparity there was an even contribution from the two factors. Each parameter uniquely accounted for 30% to 34% of the variance. For uncrossed disparity the differences in efficiency were responsible for more of the threshold variation. Adding efficiency to the equivalent internal noise prediction provided a greater increase in R
2 compared with adding equivalent internal noise to the efficiency prediction (32% vs. 20%).
Having looked at model parameters within a disparity direction, we can now compare the parameters between crossed and uncrossed relative disparity. Equivalent internal noise and processing efficiency for each disparity direction were calculated from the data shown in
Figure 3. The parameters for the two directions are plotted against each other in
Figure 5. Data points on the gray diagonal unity line indicate equal values for crossed and uncrossed disparity. Symbols falling below the unity line have higher parameter values for crossed disparity. Those above the line indicate higher uncrossed disparity values. The equivalent internal noise parameters for the two directions were correlated, but the efficiencies were not. The symbol locations in
Figure 5 can explain differences between the crossed and uncrossed disparity data in
Figure 3. Most subjects with significant differences in thresholds without external noise had roughly equal equivalent internal noise for the two directions (
Figure 5A). The only exception was subject 32. For all other subjects showing differences in sensitivity to crossed and uncrossed disparity, these were explained by efficiency differences (
Figure 5B). For subject 32, it seems a combination of both factors is responsible for the difference in sensitivity.
The two parameters in the linear amplifier model have opposing effects on the noiseless threshold. A greater equivalent internal noise for one of the two relative disparity directions will result in an increase in threshold for that direction. This increase in noise could, however, be counteracted by a reciprocal increase in efficiency. This may result in no net change. Several subjects who did not have noiseless threshold differences between crossed and uncrossed disparity are far from the unity line in
Figures 5A and B. We hypothesize that these subjects may have balanced reciprocal differences in both equivalent internal noise and efficiency. We analyzed crossed:uncrossed equivalent internal noise and efficiency parameter ratios for each subject (
Figure 6). If the two ratios were calculated based on the same data, we would expect some correlation between them. Any measurement error associated with the thresholds will affect the fitted parameters. Because the parameters interact, this error will have correlated effects on them both. To avoid this, we split the data into two subsets. We went through the list of noise mask levels and assigned each to either the odd set (0, 32, 128, and 512 arcsec) or the even set (4, 64, and 256 arcsec). We fit the linear amplifier model to each set. This gave us the equivalent internal noise and efficiency parameters for the two sets. We first compared the parameters obtained from fitting to the data from the two sets. This was to verify that the parameters obtained from fitting to the odd set were similar to those obtained by fitting to the even set. There was a highly significant correlation for both equivalent internal noise (
R2 = 59%,
p < 0.001) and for processing efficiency (
R2 = 80%,
p < 0.001). This further serves as a validation of our modeling approach. Fits to data at the odd noise levels are highly predictive of the results at even noise levels. We then examined the correlation between each parameter from the odd set with the other parameter from the even set. These ratios were significantly correlated. Individuals with increased equivalent internal noise for one disparity direction also tended to have higher processing efficiency for that direction. We can therefore split subjects into three groups: (i) those without significant differences between crossed and uncrossed disparity processing, (ii) those with balanced shifts in linear amplifier model (LAM) parameters that yield no net change in noiseless thresholds, and (iii) those whose unbalanced shifts result in threshold differences between crossed and uncrossed disparity.
We performed additional control experiments to assess the possible role of stimulus duration, and refractive error on our results. These are reported in full in our
Supplementary material. We found that reducing the stimulus duration from 250 ms to 50 ms (Experiment 3) did not change our findings. We also found a correlation between binocular visual acuity and stereoacuity, in agreement with previous reports (
Bosten et al., 2015). Surprisingly, we found no significant correlation between equivalent internal noise and binocular visual acuity. Instead, there was a significant positive correlation between processing efficiency and binocular visual acuity. Subjects with better visual acuity were better at processing the noisy disparity information. To investigate this relationship, we retested three participants without their optical correction. This allowed us to see the effect of reduced visual acuity. Several studies have shown a reduction of stereoacuity on disturbance of visual acuity (
Costa, Moreira, Hamer, & Ventura, 2010;
Hess, Hong Liu, & Wang, 2002;
Odell, Hatt, Leske, Adams, & Holmes, 2009). We found most of the effect of decreasing acuity was to increase equivalent internal noise. There was also a relatively modest reduction in processing efficiency.