OCT imaging was performed in one eye from each of the 34 BCM patients. Cross-sectional images of the retina were captured by using mainly spectral-domain OCT (SD-OCT) devices (RTvue-100; Optovue, Inc., Fremont, CA, USA) and, in a few instances, time-domain OCT (TD-OCT) instruments (OCT1, OCT3; Carl Zeiss Meditec, Dublin, CA, USA) as described.
10 Briefly, overlapping 4.5- or 9-mm scans were taken along the horizontal and vertical meridians through the fovea. Segmentation analysis was performed with custom computer programs (MatLab 7.5; MathWorks, Inc., Natick, MA, USA), and signal peaks corresponding to retinal laminae were assigned on the basis of previously published work.
13–16 The foveola was identified as the maximum depression on the scans, and foveal outer nuclear layer (ONL) thickness was analyzed as in previous works.
10 Scans from normal subjects (
n = 22; age range, 8–62 years) for comparison with those of patients have been previously published and include a normal subset (
n = 15) with spherical errors of +2 to −4 diopters (D), and a subset (
n = 7) with higher degrees of myopia (−5 to −10 D).
10 ONL and rod outer segment (ROS) thicknesses were measured at the rod hot spot, a rod-rich region 10° to 16° (3–5 mm) eccentric to the fovea in the superior retina.
17 Each was defined as the average of five measurements taken at 0.5° intervals over a region 10.5° to 12.5° eccentric to the fovea in the superior retina.
18 ONL thickness was plotted at the fovea, and a generalized additive model was used to describe photoreceptor loss over time.
19 To take into account multiple recordings from the same subject, random effect was incorporated in the model, and rate of decay was calculated from this model. Statistical analysis was performed by using R statistical computing software (version 3.4.4; Vienna, Austria). The extent of the disruption of the hyperreflective layer demarcating the inner segment/outer segment (IS/OS) line was analyzed; horizontal raster scans of the macula (6 × 6 mm, 101 B-scans, 513 A-scans) were obtained with SD-OCT; and several single scans going through the fovea (4.5 mm) with TD-OCT. Extent of disruption of the IS/OS line was measured as the distance between edges of intact IS/OS. In cases of multiple disruptions over the area, the longest extent was taken. To be noted, axial length estimates were not available; however, all lateral distances are presented in terms of visual angle, which is expected to be independent from ocular magnification differences between patients.