The PTM (Lu & Dosher,
1998) has been used extensively to model the effects of attention on contrast sensitivity. We apply it here to understand the signal-detection mechanisms underlying intrasaccadic suppression. The model includes an input stage (
Figure 2a), a set of signal-processing stages (
Figure 2b through d), and an output (
Figure 2e) resulting in a decision variable (DV). The elegance of the PTM lies in the qualitatively distinct changes in TvN curves predicted for variations of the parameters that represent each of the processing stages (
Figure 2b through
d). We applied the PTM to detection thresholds obtained during saccades and during fixation with the goal of ascertaining which of the processing stages were responsible for intrasaccadic suppression.
The PTM implemented here consists of two identical spatial channels: one for the screen location that receives signal-plus-noise and one for the screen location that receives only noise (
Figure 2a). The variable
c represents signal contrast (or strength). The
α parameter is a novel addition to the PTM, which we discuss below. Each of the spatial channels proceeds independently until the final stage, at which their outputs are subtracted (
Figure 2e) to produce the DV. If the DV is greater than zero, then the model responds that the signal was in the upper screen position. If the DV is less than zero, then the model chooses the lower screen position. DV's distribution has a total variance (
Display Formula ) that can be expressed as a function of the external noise (noise added to the signal before it enters the system) and the model parameters. The detector's sensitivity (
d′) is then given by the ratio of the signal,
βc/(1 +
α), and the standard deviation of the DV,
σt. Analogous to the derivation in Watson and Krekelberg (
2011; their equations 1–3), this allows us to express the contrast threshold for a given level of performance (
d′) as a function of external noise (
σe) and the model parameters
Figure 3 shows the shape of TvN curves that the PTM predicts if intrasaccadic suppression is determined by a change in only one of the parameters or dominated by that parameter. In other words, these are the quantitative hypotheses that our experiments tested.
The first processing stage is the perceptual template stage (
Figure 2b). This stage's output depends on how well the template matches the input signal, in effect, modeling selectivity. The template's two features are a gain parameter (
β) and a tuning parameter (
w) controlling the width of the template. The gain (
β) amplifies the input, which contains either signal plus external noise (
Figure 2a, top) or noise only (
Figure 2a, bottom). The template can be thought of as an exclusion term: In general, a tighter template (a smaller
w) implies a more focused perceptual analysis on the true timing, spatial position, or other characteristic (e.g., spatial frequency) of the stimulus (Lu & Dosher,
1998). In our model, an increase in the template stage (
w) refers to an increase in spatial uncertainty about the signal. A narrow template (less spatial uncertainty) focuses the detector on only the relevant spatial location and thereby excludes any external noise appearing outside of the signal's location. Therefore, an increase in external noise has a minimal effect on thresholds for a narrow template. Now consider a wide template: External noise existing outside of the signal's location would be allowed into the detector. At low external noise levels, this would have only a minimal influence on thresholds. However, at high external noise, the wider template's inclusion of noise would have a dramatic effect on thresholds (
Figure 3a), allowing high levels of noise (outside of the signal's location) into the detector. Therefore, if saccadic suppression occurs because of an increase in spatial uncertainty, we expect saccade and fixation thresholds to diverge as external noise increases (
Figure 3a).
The second processing stage is a multiplicative noise injection (
Figure 2c). The noise added to each channel at this stage is stimulus dependent because the output of the template stage is scaled by the parameter (
σm). Because this noise injection is scaled by both the signal and noise, the PTM predicts that detection thresholds will be influenced equally at both low and high external noise levels (
Figure 3b). Therefore, if saccadic suppression is caused by a stimulus-dependent noise injection, we expect a constant amount of suppression (in log units) across external noise conditions.
The third stage is a stimulus-independent additive noise injection (
Figure 2d). Noise with standard deviation
σa is added to the system, independent of the signal or external noise. It follows that as the external noise is increased, this term will have less of an influence on the threshold. Therefore, the PTM predicts that varying this term will lead to different thresholds at low external noise, when the internal noise is dominated by this additive injection. As external noise is increased (thereby increasingly influencing the system's response) while the additive noise remains constant, the thresholds should converge (
Figure 3c). Because this term is mathematically equivalent to gain (
β) reduction (see
Equation 1), we will consider its effects under the gain (
β) parameter.
To model the possible influence of receptive field (RF) shifts that are known to occur at the time of saccades (Duhamel et al.,
1992; Tolias et al.,
2001), we introduced a novel parameter into the PTM. A spatially shifted detector should reduce the signal but not the external noise (assuming the shifted position is also somewhere on the display); hence, we introduced the term at the earliest stage (
Figure 2a). The parameter (
α) represents the amount of shift between the detector and the stimulus (when there is no shift,
α equals zero, and the input to the detector is equal to
c). Our simulation of the influence of
α (
Figure 3d) shows a trend similar to that of multiplicative noise injection (
Figure 3b). Because it is qualitatively similar to multiplicative noise injection (
σm), we do not consider
α in the fits.