A conventional classification image is a composition of a set of classification subimages. A subimage CI
AB is the average of all the noise patterns
N σ (
Equation 1) from trials where the signal in the stimulus was
A and the observer's response was
B. Consider the two-letter identification task (“O” vs. “X”). The subimage CI
OX is the average of the noise patterns
N OX from trials where “O” was in the stimulus but the observer responded “X” (we refer to this as an OX trial). An “X” response implies that the internal decision variable for an “X” response was greater than that for an “O” response; that is,
λ(“X”) >
λ(“O”). Appealing to the uncertainty model (
Equation 7) and the composition of a stimulus (
Equation 1) and letting
X j =
T x,j and
O j =
T o,j to improve readability, we have
where
O (without any subscript) is the “O” signal in the noisy stimulus presented to the observer. If there is no uncertainty (
M = 1),
Equation 11 becomes the familiar form that underlies the conventional classification image:
The right-hand side of the inequality is a positive number because a noiseless “O” stimulus will activate the “O” channel (
O 1) more than the “X” channel (
X 1); that is,
O T O 1 >
O T X 1. For this inequality to hold, the average noise pattern on the left-hand side must have a positive correlation with the X template and a negative correlation with the O template. Ahumada (
2002) showed analytically that
where
E[·] denotes a mathematical expectation (see also Abbey & Eckstein,
2002; Murray et al.,
2002). The proportional constant is affected by the probability of an OX trial (stimulus “O,” response “X”), and the internal-to-external noise ratio (ratio between the variances of the noise internal to an observer and that in the stimuli; e.g., see Equation A3 in Murray et al.,
2002). CI
OX approaches
E[
NOX] as the number of OX trials (
NOX) approaches infinity. For a finite number of trials, the variance of CI
OX is rather cumbersome because the probability density of CI
OX is a truncated version of the multidimensional Gaussian (
Nσ) used to form the stimuli. Ahumada (
2002) pointed out that the variance of CI
OX is upper bounded by the variance of the nontruncated distribution. Murray et al. (
2002, Appendices A and F) further argued that the difference between the upper bound and the actual variance is negligible for a typical classification-image experiment where (1) the amount of the stimulus noise is comparable to the level of the observer's internal noise, (2) the number of independent image pixels (and hence the dimensionality of stimulus) is large, and (3) the accuracy level is above 75%. All of the experiments in the current study met these three conditions. Thus, CI
OX can be approximated as
where
Nσ is a sample of white noise from the distribution used to form the stimuli (
Equation 1).