In experiment 1, the mean RTs from all trials were collected for further analysis. The results revealed nonsignificant main effects of target type (
F(1, 23) = 1.301,
p = 0.266,
ηp² = 0.054) and SF of gratings (
F(1, 23) = 0.248,
p = 0.623,
ηp² = 0.011), as well as a nonsignificant interaction between the two factors (
F(1, 23) = 0.493,
p = 0.490,
ηp² = 0.021; see
Figure 2A). Further analysis showed that manual RTs for threatening stimulus were comparable to nonthreatening stimulus under both LSF (
t(23) = −1.473,
p = 0.154,
d = 0.301) and HSF (
t(23) = −0.372,
p = 0.713,
d = 0.076) conditions.
In experiment 2, trials with saccades faster than 50 ms and slower than 350 ms (1.6% of all trials), and trials with saccade peak velocity slower than 50 degrees/second (0.5% of all trials), as well as trials with the end position of saccades outside the target area (undershoot or overshoot; 9.4% of all trials) were excluded from further analysis. For saccade latency, the main effect of target type was significant (
F(1, 23) = 7.260,
p = 0.013,
ηp² = 0.240), but the main effect of SF of gratings (
F(1, 23) = 0.005,
p = 0.945,
ηp² = 0.000) and the interaction between the two factors (
F(1, 23) = 3.496,
p = 0.074,
ηp² = 0.132) failed to reach significance. Further analysis showed that saccade latency for threatening stimulus was significantly shorter than for nonthreatening stimulus under LSF condition (
t(23) = −2.949,
p = 0.007,
d = 0.602; see
Figure 2B), instead of HSF condition (
t(23) = −1.519,
p = 0.142,
d = 0.310). For average saccade velocity, the main effect of SF of gratings was nonsignificant (
F(1, 23) = 0.489,
p = 0.491,
ηp² = 0.021), but the main effect of target type (
F(1, 23) = 16.477,
p < 0.001,
ηp² = 0.417) and the interaction between the two factors (
F(1, 23) = 6.429,
p = 0.018,
ηp² = 0.218) were significant. Further analysis showed that saccade velocity was significantly faster for threatening stimulus than for nonthreatening stimulus under LSF condition (
t(23) = 4.571,
p < 0.001,
d = 0.933; see
Figure 2C), instead of HSF condition (
t(23) = 1.662,
p = 0.110,
d = 0.339).
In experiment 3, the main effect of SF of gratings was not significant (
F(1, 23) = 0.723,
p = 0.404,
ηp² = 0.030), but the main effect of target type (
F(1, 23) = 9.845,
p = 0.005,
ηp² = 0.300) and the interaction between the two factors (
F(1, 23) = 7.998,
p = 0.010,
ηp² = 0.258) were significant. Further analysis showed that reaching RTs for threatening stimulus were significantly faster than for nonthreatening stimulus under LSF condition (
t(23) = −4.091,
p < 0.001,
d = 0.835; see
Figure 2D), instead of HSF condition (
t(23) = −1.190,
p = 0.246,
d = 0.243).
To directly compare the threat advantage (RTnon-threat − RTthreat) among the three experiments, we log10 transformed the data and calculated the threat advantage for both LSF and HSF conditions. The results showed that the main effect of response type was significant for LSF condition (F(2, 69) = 3.393, p = 0.039, ηp² = 0.090), but was not significant for HSF condition (F(2, 69) = 0.451, p = 0.639, ηp² = 0.013). Bonferroni pairwise comparisons revealed that the threat advantage under LSF condition was significantly larger for saccade responses than for manual responses (p = 0.034), whereas the threat advantage for reaching responses was comparable to that for saccade responses (p = 0.746) and manual responses (p = 0.466).