Kollbaum Pete S, Bradley Arthur, Thibos Larry N
School of Optometry, Indiana University, Bloomington, IN, USA.
Optom Vis Sci. 2013 Sep;90(9):924-36. doi: 10.1097/01.opx.0000434275.93435.da.
The purpose of the current study was to examine the on- and off-eye optical performance of two types of soft contact lenses (hydrogel and silicone hydrogel).
The monochromatic aberrations (λ = 850 nm) of contact lenses were measured on-eye using a clinical Shack-Hartmann ocular aberrometer. In addition, we used an off-eye single-pass contact lens aberrometer (λ = 540 nm) in which the soft contact lens was placed within a wet cell. Comparison of the lower and higher order aberrations measured with these two methods required compensation for different wavelengths and knowledge of the refractive index of the contact lens materials.
The measured on-eye sphere and spherical aberration values were generally similar to those measured off-eye and those specified by the lens manufacturers for both types of soft contact lenses. However, there were notable differences, especially for high plus-powered lenses, which typically exhibited lower sphere power on the eye than expected from the lens specifications and from the off-eye measured powers, both of which were almost identical. Longitudinal spherical aberration varied with lens power in the hydrogel lenses, as expected from geometric optics theory. Longitudinal spherical aberration measurements on- and off-eye, however, deviated significantly from that expected of a thin lens with spherical surfaces due to surface asphericities. The difference between on- and off-eye optics can be modeled as a tear lens or as relative lens thickness changes caused by lens flexure.
The results of the current study reveal that the major difference between the on-eye lens optics and the manufacturers' specifications is not due to lens errors but due to eye-lens interactions, which could be either lens flexure or a tear lens forming behind the soft contact lens.
本研究旨在考察两种类型的软性隐形眼镜(水凝胶和硅水凝胶)在眼上和眼外的光学性能。
使用临床Shack-Hartmann眼像差仪在眼上测量隐形眼镜的单色像差(λ = 850 nm)。此外,我们使用了一种眼外单通道隐形眼镜像差仪(λ = 540 nm),将软性隐形眼镜置于湿盒中。用这两种方法测量的低阶和高阶像差进行比较时,需要对不同波长进行补偿,并了解隐形眼镜材料的折射率。
对于两种类型的软性隐形眼镜,测量得到的眼上球镜度和球差值通常与眼外测量值以及镜片制造商规定的值相似。然而,存在显著差异,特别是对于高正度数镜片,其在眼上的球镜度通常低于镜片规格和眼外测量度数所预期的值,而这两者几乎是相同的。正如几何光学理论所预期的,水凝胶镜片的纵向球差随镜片度数而变化。然而,由于表面非球面性,眼上和眼外的纵向球差测量值与具有球面的薄透镜所预期的值有显著偏差。眼上和眼外光学之间的差异可以建模为泪液透镜或由镜片弯曲引起的相对镜片厚度变化。
本研究结果表明,眼上镜片光学与制造商规格之间的主要差异不是由于镜片误差,而是由于眼 - 镜片相互作用,这可能是镜片弯曲或在软性隐形眼镜后方形成泪液透镜。