Previous studies have demonstrated that Vernier displacement thresholds determined from 1F responses reflect Vernier acuity (Norcia et al.,
1999), whereas the spatial frequency threshold at all harmonics of grating on/off responses reflect grating acuity (Hou et al.,
2015; Tang & Norcia,
1995). Thus, we focused on the analysis of the 1F component.
Figure 4 plots the 1F responses as a function of the swept parameters in different visual ROIs, averaged coherently across all participants. The data of one of 13 participants in the spatial frequency sweep paradigm were excluded because of low signal-to-noise ratio. The solid lines represent fits to the data of a generalized Naka-Rushton equation,
y =
axn/(
xn +
bn), where
a is the maximum amplitude,
b is the semisaturation constant, and
n is the exponent. A separate one-way (ROIs) ANOVA for each fit parameter of the Vernier and grating response showed no significant difference, except for
b of Vernier stimuli (
p < 0.0001; see
Table 2). A further paired
t test of the Vernier semisaturation constant showed significantly lower values in V1 and LOC than in hMT+ and hV4 (with Bonferroni correction) but no significant difference between V1 and LOC or between hV4 and hMT+ (
Table 3). Because the semisaturation constant (
b) value reflects the sensitivities of the response functions, we define it as the “response threshold.” The response threshold measure for detecting Vernier displacement indicates that cortical areas V1 and LOC are particularly sensitive to near-threshold Vernier displacements, whereas cortical areas hV4 and hMT+ are less sensitive. This sensitivity difference between ROIs to Vernier stimuli can be seen clearly in the left panel of
Figure 4, where the arrows point to the semisaturation constant (response threshold) in each ROI. In contrast, all ROIs (V1, LOC, hV4, and hMT+) showed similar sensitivity to near-threshold spatial frequencies (see
Figure 4, right panel).