Models with transduction nonlinearities and stimulus-dependent noise are often equivalent to linear models with stimulus-independent noise, if the range of relevant stimuli is small compared to the range over which the transduction nonlinearities and stimulus-dependent noise amplitudes change appreciably (
Ahumada, 1987). To take just one example, in
Foley and Legge’s (1981) model of grating detection and discrimination, observers use a decision variable with mean
and fixed variance, where
c is the signal grating contrast and
c0 is an arbitrary reference contrast. This is clearly a nonlinear model, but in a task where the observer discriminates between two gratings of fixed contrast
cA and
cB, the nonlinearity can be accommodated within the noisy cross-correlator model. Let
I be a unit-contrast grating, so that
cI is a grating of contrast
c. We can incorporate
Foley and Legge’s (1981) power-law transduction nonlinearity by writing the decision variable in response to a stimulus
cI+
N as
. With no external noise, this decision variable has mean
and fixed variance, as in
Foley and Legge’s (1981) model. If the external noise
N causes the term
to vary over only a small range, as in an experiment where observers discriminate between gratings of similar contrasts
cA and
cB, we can use a Taylor series approximation that is linear in the external noise term
N:
. If we rescale the decision variable, multiplying by
, we can rewrite it as
. As we pointed out when we discussed early and late noise, we can choose
Z so that
, and rewrite the decision variable as
. Hence over a small contrast range, the observer behaves like a noisy cross-correlator, except that the internal-to-external noise ratio depends on the signal contrast
c. When an observer discriminates between gratings of two similar contrasts
cA and
cB, the internal noise power will be approximately the same on signal-
A and signal-
B trials, and the methods we have derived will be approximately optimal. When the grating contrast ratio
cAcB is very different from 1, as when
cA or
cB is zero in a detection experiment, the internal-to-external noise ratio may be very different on the two types of trials. As we pointed out in our discussion of proportional noise, the methods we have derived can be easily modified to handle this case as well.