The four learning functions differed only in the rate of learning: the (1λ - 4 β - 1 α) model provided an excellent fit with rates of: βs = 1.1478, 1.3763, 1.7446, and 2.3077 (λ = 1.0984, and α= 0.0713) for zero noise (
r2= 0.9411) and βs = 0.5538, 0.7936, 1.3242, and 1.2836 (λ = 0.8979, and α= 0.3262) for high external noise (
r2 = 0.9554), listed for
All,
Near,
Far, and
Single, from slower to faster. A lattice of subcase models and nested significance tests rejected more complicated models (see the discussion in
Appendix A, 2, and
Tables A.1 and
A.2). The SDs of the estimated parameters, computed using bootstrap methods, are listed in
Table A.3. The parameter SDs are relatively large (reflecting slight threshold level differences between observer groups and parameter correlations; added variance from parameter correlations was partially discounted in SDs of normalized rates). Despite this, the ordinal consistency of the four rates from the bootstrapped methods, which is perhaps more meaningful, was very high. For example, in zero noise, β
All was slower than β
Single, slower than β
Far, and slower than β
Near in 998, 949, and 786 fits, respectively, out of 1,000 fits to resampled data sets; and in high noise, β
All was slower than β
Single in 1,000 fits, slower than β
Far in 1,000 fits, and slower than β
Near in 950 fits out of 1,000 fits to resampled data sets (ordinal statistics are also listed in
Table A.3). Consistent with the ANOVA tests, in high noise, β
Far is slower than β
Single only in 469 out of 1,000 fits—they are not significantly different from each other.