25 light-point-array positioned at a R1-R6’s receptive field center, generating two bright front-to-back moving dots. (
A) Characteristic responses of a R1-R6 at 25°C to the dots, 1.7, 3.4 or 6.8
o apart, travelling 102
o/s in front-to-back direction. (
B) Individual outputs resolved the dots, which were less than the interommatidial angle (Δφ = 4.5
o) apart (yellow box); resolvability given by the Raleigh criterion (
Figure 7C). Microsaccadic sampling model (
Figure 9) predicted a comparable resolvability threshold (dotted line). (
C) At lower dot velocities (20–50
o/s), corresponding to normal gaze fixation speeds in close-loop flight simulator experiments (Appendix 10), each R1-R6 responded to the tested hyperacute dot separations (1.7
o and 3.4
o) even stronger. Notice the small staircase-like steps in voltage responses. These represent light from 25 individual light-guide-ends being turned on/off in sequence to generate the moving dots, crossing the receptive field slowly (see Appendix 6). (
D) At 20
o/s velocity, neural resolvability to the tested hyperacute dot separations was between 10–20%. (
E) R1-R6 output to the two dots, having the same separations as above, but now moving at fast saccadic velocity (409
o/s). (
F) Although, at such a high speed, R1-R6 output could not resolve the hyperacute dot separations (1.7
o and 3.4
o) consistently, the dots were nevertheless clearly detected when at 5.1
o apart (cyan bar), which is about Δφ.