The majority of previous studies performed to determine individual variability in foveal shape have used direct measurement obtained from OCT devices. In our study, we used a fitted a mathematical model proposed by Scheibe et al.
11 to the images because being able to determine shape at many different locations across the whole macular is important for structure–function mapping.
10 In our previous study, we used the same model to estimate the shape of the GCL+IPL for the purpose of customized structure–function mapping in the macula. Briefly, the model is “one-sided,'' modelling a curve from the fovea out to the more peripheral retina as the sum of two exponential functions. The first function has three parameters that control the location, height, and steepness of the rim. The second function makes use of the width and steepness parameters, and has a fourth weighting parameter that is the height of the retina outside the fovea. By fitting these four parameters to minimize the sum-of-square differences between the function and one-half of the OCT profile, one has a simple formula that describes the profile, allows easy extraction of measurements, and can be readily interpolated to other meridians of the macula.
Figure 2C shows an example of the fitted model.
In this paper, we are interested in the total foveal shape profile, so we fit the model to the entire retinal thickness profile, not just the GCL+IPL. To obtain this total foveal shape profile, from the Spectralis .vol file we subtracted the ILM profile as segmented by the Spectralis software from the RPE profile as given by the Spectralis. After obtaining this total retinal profile, the point of minimum thickness was calculated by scanning from the left and right while the difference is decreasing, and taking the minimum of the two. This point was considered as the center of the scan. This process is shown in
Figure 2, where the ILM and RPE are taken from
Figure 1 (
Fig. 2A), the difference taken (
Fig. 2B), and the minimum of that difference used to find the midpoint of the scan (
Fig. 2B). The scan was divided in two, and the four-parameter Scheibe model fitted to each half (
Fig. 2C). While this fitted curve is important for structure–function modelling, in this paper we are interested in three measurements: the central thickness (an estimate of the ILM-RPE difference at the point of minimum thickness;
Fig. 2A), the maximum thickness (an estimate of the IPL-RPE difference at its highest computed as “Height” in
Fig. 2C plus “Central thickness” from
Fig. 2A), and the radius, corresponding to the distance between the center of the scan and the point of the maximum thickness (
Fig. 2C).