Figure 2a,
b plots the proportion of synchrony responses for each tone-relative disk onset time (SOA) in each of the three adaptation lag conditions (−106, 0, and 106 ms). An SOA of 0 ms refers to the single disk within a given trial's display whose luminance modulation is physically synchronized with the tone. Negative test SOA values represent disks whose luminance increments are lagged relative to the onset of the tone; positive SOAs indicate disks with luminance increments that precede increments in tone intensity. Synchrony responses in each of the six adaptation conditions were fitted with a Gaussian:
Here, A represents the amplitude, and SD is the standard deviation corresponding to the precision of audiovisual simultaneity estimates. PSS, the key parameter of interest here, is the defined as the lag (test SOA) associated with the fitted Gaussian's peak.
Mean estimates of PSS for each adaptation condition are plotted in
Figure 2b. A highly significant main effect of adaptation lag was observed on PSS,
F(2, 5) = 81.889,
p < 0.001. To examine which audiovisual lags exerted shifts in PSS relative to the synchronous audiovisual adaptation condition, we conducted two separate pairwise repeated-measures
t tests: All audiovisual asynchronies generated significant shifts in PSS relative to synchronous adaptation conditions: −106 ms lag:
t(5) = −4.414,
p = 0.007; +106 ms lag:
t(5) = −9.036,
p < 0.001. Separate within-subjects ANOVAs failed to find significant differences in fitted
SDs or amplitudes across the different adaptation conditions,
SD:
F(2, 5) = 1.79,
p = 0.278;
A:
F(2, 5) = 0.548,
p = 0.616. Visual inspection of individual data in
Figure 2a reveals that the comparatively large mean
SD value obtained in the +106 lag adaptation was largely a consequence of poor performance from a single observer in this condition (see Subject 2 in
Figure 2a).
To examine whether the adaptation period itself had any effect on PSS (accuracy),
SD (precision), or amplitude, we fitted synchrony performance measured without periods of lag adaptation (Van der Burg et al.,
2014). Mean estimates of each fitted parameter are plotted in
Figure 2b through
d (see horizontal dashed lines). A Mann–Whitney U test failed to find a significant difference between estimates of PSS derived under unadapted and physically synchronous (0-ms lag) adaptation conditions (
p = 0.792). Two separate independent samples Kruskal-Wallis tests comparing fitted estimates of Gaussian
SD and
A indicated that neither parameter varied across any condition tested (unadapted, −106, 0, and +106 ms lag adaptation),
SD:
p = 0.916;
A:
p = 0.840.
This is the first demonstration of TR using an audiovisual synchrony search task within a highly cluttered visual environment (Van der Burg, et al.,
2014). Expressed as a proportion of the adapted lag, PSS shifts rarely exceed 50% (Fujisaki et al.,
2004; Heron, Roach, Hanson, McGraw, & Whitaker,
2012; Vroomen et al.,
2004). Our experiment yields larger shifts in PSS (∼75 ms, tone leading; 120 ms, flash leading) corresponding to shifts of 70% and 115% of the adapted lag respectively. One possible reason we observe such large shifts may be that the search task itself is rather difficult. Although on any given trial one of the visual search objects was always synchronized with the tone, the temporal proximity of other objects (those with temporally adjacent modulation phase) may spuriously bind with the auditory signal. Indeed, spurious audiovisual bindings are frequently observed in spatiotemporally cluttered visual contexts when competing visual events occur within ∼80 ms of the auditory event; the so-called window of simultaneity (Van der Burg, et al.,
2014; Van der Burg, Cass, Olivers, Theeuwes, & Alais,
2010; Van der Burg, Olivers, Bronkhurst, & Theeuwes,
2008).