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. 2024 Jul 18;15:1328853. doi: 10.3389/fpsyg.2024.1328853

Table 2.

Parameter estimates of the LMM for RTs in Experiment 1.

Parameter Estimate SEM df t p 95% CI
Lower Upper
Constant Term 2008.033333 134.477797 3,156.000 14.932 0.000 1744.360573 2271.706094
GROUP −630.791954 155.949466 3,156.000 −4.045 0.000 −936.564557 −325.019351
BLOCK −300.133333 190.180325 3,156.000 −1.578 0.115 −673.022927 72.756261
QUANTIFIER −8.613978 188.640378 3,156.000 −0.046 0.964 −378.484174 361.256217
[PROPORTION = 20] −124.885185 195.391710 3,156.000 −0.639 0.523 −507.992824 258.222454
[PROPORTION = 30] 29.395238 193.546610 3,156.000 0.152 0.879 −350.094684 408.885160
[PROPORTION = 40] 85.735897 197.359450 3,156.000 0.434 0.664 −301.229922 472.701717
[PROPORTION = 50] 239.600000 190.180325 3,156.000 1.260 0.208 −133.289594 612.489594
[PROPORTION = 60] −43.343678 191.812804 3,156.000 −0.226 0.821 −419.434100 332.746743
[PROPORTION = 70] −100.783333 187.185172 3,156.000 −0.538 0.590 −467.800283 266.233616

Note that only the parameters for the main effects are reported here, since the sole focus is on the polarity effect. The full list of parameters can be found in Appendix A1.