We presented a plaid stimulus composed of two square-wave gratings through a circular aperture, about 13° in diameter, on a black background, as shown in
Figure 1a. The luminance of the black background outside the aperture was 0 cd/
\(\rm {m^2}\). The two gratings had normal directions
\(\theta _1\) and
\(\theta _2\). The plaid moved at speed
\(v=\) 5°/s in the direction
\(\theta =\) 45° (from the lower left corner of the screen to the upper right corner).
\(\Delta {\theta _1}=\theta _1-\theta =\) −60° and
\(\Delta {\theta _2}=\theta _2-\theta =\) −75.5° define the relative directions of the individual gratings with respect to the direction of the plaid. With this geometric arrangement, the ratio between the two gratings speeds is
\(\cos \Delta {\theta _1}/{\rm cos} \Delta {\theta _2}\). In particular, stimuli were designed as plaids, whose direction fell outside the range of the directions of the two component gratings (type II plaid; see
Ferrera & Wilson, 1990). We chose gratings directions that were relatively close to one another, and far away from the direction of the whole plaid pattern. Because of this geometric arrangement the plaid motion direction was distinct from that of the gratings (
Cropper et al., 1996), and the directions of gratings were sufficiently close to one another to be interchangeable with their average. Each grating was composed of dark (55–65 cd/
\(\rm {m^2}\)) and light (115–125 cd/
\(\rm {m^2}\)) stripes, and a spatial frequency of 0.6 cycle/°. Stimulus was presented in transparency (
Stone et al., 1990;
Stoner et al., 1990;
Stoner & Albright, 1992), and the perceptual uncertainty was modulated by varying the contrast level of each grating. The overall plaid image was defined as:
\begin{eqnarray*}
L({\boldsymbol{x}},t)=L_0 [1+C_1 g_1({\boldsymbol{x}},t)+C_2 g_2({\boldsymbol{x}},t)],
\end{eqnarray*}
where
\(L_0\) is the mean intensity,
\(g_1\) and
\(g_2\) are the functions that defined the two component gratings, and
\(C_1\) and
\(C_2\) are the gratings’ contrast levels, respectively (
Stoner et al., 1990). The total contrast
\(C = C_1 + C_2\) was kept constant, and the relative contrast difference between the gratings of each plaid was defined as
\(\Delta {c}=|C_1-C_2|/C\). In all experiments, we set
\(L_0\simeq \rm 90\, cd/m^2\) and
\(C = 0.5\). Participants were instructed to maintain fixation at the center of the stimulus during the entire duration of stimulus presentation. Stimuli were generated using Psychophysics Toolbox for Matlab (
Brainard, 1997;
Kleiner et al., 2007).