M-scaling was originally conceived as reflecting the scaling properties of the primary, retino-cortical visual pathway, and the inverse-linear cortical magnification rule can be restated using
E2 as
where
M0 is the foveal cortical magnification factor and
E2 is Levi's value (at which
M−1 doubles in this case). Two implications of the M scaling analogy and retinotopic mapping should be considered: (a) given retinotopic mapping with an
M scale: what is the locus of the flankers in the primary visual cortex? (b) Is an asymmetry of the flanker interaction compatible with this framework? Pelli (
2008,
Equation 3) derived an answer to question (a) which states that, if spacing in a crowding task is proportional to eccentricity (i.e., if it obeys Bouma's rul
e as in
Equation 3), then the flankers appear at
fixed spacing at the primary visual cortex. Now, however, Pelli's derivation is based on the logarithmic mapping (of visual space onto the cortex,
δ ∝ ln
E) derived by Schwartz (
1980), which Schwartz, for simplicity, based on the proportionality assumption. The logarithmic mapping has been repeatedly verified to hold for eccentricities larger than about 3° eccentricity but is not meant for and is not valid at small eccentricities (Strasburger et al.,
2011; see there for the derivations of the following equations). It is, in particular, undefined in the fovea. Fortunately, the reasoning can be generalized by using the standard inverse linear cortical magnification rule (
Equation 10). Under this rule, one can derive that (in analogy to Schwartz's mapping) the cortical distance
δ of the target from the fovea is
with notations as before (note that, unlike the original logarithmic mapping, this equation is well-defined in the fovea). With
Equations 10–
12 one can then derive how critical spacing on the cortex, Δ
δ varies with eccentricity:
where
E2 refers to local size (
Equation 11) or to distance from the fovea (
Equation 12), and
Ē2 refers to critical spacing in
Equation 10. Different symbols are used for
E2 from
Equations 10 and
11 since the variation of local size and location on the one hand, and of critical spacing on the other hand are likely different. The behavior of
Equation 13 depends on the ratio
E2/
Ē2. The foveal value Δ
δ0 is given by
From that foveal value, cortical critical spacing Δ
δ either increases
or decreases with increasing eccentricity, depending on that ratio. For eccentricities larger than both
E2 and
Ē2, however,
Equation 13 quickly converges to the value
i.e., becomes constant.