Here we measured OLRs using our previously described head-fixed paradigm (
Kirkels et al., 2018) to investigate whether mice perceive reverse-phi stimuli. Mice respond to changes in direction for phi stimuli and reverse-phi stimuli in opposite ways. Displacement of dot patterns in phi stimuli caused mice to reflexively compensate and adjust their running direction to the direction of the moving pattern. For the reverse-phi stimulus, however, mice responded by turning in the opposite direction to the dot displacement. This behavior is consistent with how human observers perceive phi and reverse-phi stimuli and is in accordance with psychophysical and neurophysiological findings from previous studies on reverse phi in other animals and humans (
Bours et al., 2009;
Clark et al., 2011;
Emerson et al., 1987;
Hassenstein & Reichardt, 1956;
Ibbotson & Clifford, 2001;
Krekelberg & Albright, 2005;
Livingstone & Conway, 2003;
Orger et al., 2000;
Tuthill et al., 2011).
Our results show that the responses of mice are variable. First of all, the magnitude of the OLRs to phi and reverse-phi stimuli is considerably smaller than that for the OLRs we observed to unlimited lifetime motion stimuli we used in previous work (
Kirkels et al., 2018). In the present study, the mean OLR peaks at about 15°/s with our most optimal parameter settings for perception of motion reversal, whereas our previous work reported a peak amplitude of about 30°/s. Although most parameters such as speed, contrast, and dot size were identical in these studies, an important difference was the use of single-step as opposed to unlimited lifetime for the dots, which is necessary for clean reverse-phi stimuli (
Bours, Kroes, & Lankheet, 2007). Shortened dot lifetime has a negative effect on the signal-to-noise ratio of OLRs because more noise is present in the stimulus, which results in less motion energy in one direction (
Hadad, Schwartz, Maurer, & Lewis, 2015). Two of the mice in our population showed other behavior with oppositely directed OLRs (
Figure 3), which might be a result of this stimulus noise or because the number of successfully completed trials was less than for the other mice. It is also possible that the signal-to-noise ratio is different in these mice, as not all C57BL/6J mice have a fully functioning visual system. However, it is also possible that these two mice really have oppositely directed OLRs, and the underlying reason for this opposite behavior is unclear.
We demonstrated a dependency of the OLR reversal effect on step interval. We found that the difference between the response to phi and reverse-phi stimuli is largest at a temporal interval of 33 ms. This is on the same order of magnitude as the slower delay filters mentioned in earlier studies in flies (
Brinkworth & O'Carroll, 2009;
Eichner, Joesch, Schnell, Reiff, & Borst, 2011;
Shoemaker, O'Carroll, & Straw, 2005). A more recent fly study, however, showed maximal responses around a delay of 17 ms in both behavioral and neural measurements (
Salazar-Gatzimas et al., 2016). It is important to note that results of these experiments might be specific for the chosen stimulus conditions. It has been shown in human psychophysical studies that perception of reverse-phi motion depends on many factors, such as stimulus eccentricity, spatial proximity, contrast, and spatial and temporal frequency (e.g.,
Anstis & Rogers, 1975;
Benton, Johnston, & Mcowan, 1997;
Bours et al., 2009;
Chubb & Sperling, 1989;
Edwards & Nishida, 2004;
Oluk, Pavan, & Kafaligonul, 2016;
Wehrhahn, 2006). Therefore, changes in our parameters such as dot size, step size, and stimulus speed could very well affect our finding.
Although the mean pooled OLR to reverse-phi was largest at a delay of 17 ms, the OLR to phi stimuli was almost entirely abolished at this delay. Why would the difference between phi and reverse-phi OLRs be so different at this step time? It should be noted that, to keep the dot speed always at 36°/s, the displacement from the first instance of the dot to the second was only 0.6°, or 1/5 of the dot diameter. Our data suggest that this was too small for the mouse to detect in the phi condition. In the reverse-phi condition, however, because the first and second instances are of opposite contrast polarity and displayed only briefly and in rapid succession, the overlapping parts in effect cancel each other and blend into the mid-gray background. We speculate that the strong response to the reverse-phi stimulus in this condition is driven by the black and white slivers visible at either side of this canceled-out region.