Drexler W, Hitzenberger C K, Baumgartner A, Findl O, Sattmann H, Fercher A F
Institut für Medizinische Physik, Universität Wien, Währinger Strasse 13, Wien, A-1090, Austria.
Exp Eye Res. 1998 Jan;66(1):25-33. doi: 10.1006/exer.1997.0401.
We report on quantitative measurements of group refractive indices and group dispersion in water and in human ocular media such as the cornea, the aqueous humor, the lens, artificial intraocular lenses, as well as a total value averaged over the media along the axial eye length of normal subjects and pseudophakic patients in vivo using dual beam partial coherence interferometry. Different optical thickness values due to the dispersion of the cornea are demonstrated using two spectrally displaced light sources. The displacement can be used to indirectly calculate the group dispersion of the human cornea in the spectral region between 810 nm and 860 nm. If the object under investigation is dispersive, resolution is limited due to a broadening of the detected signals. This broadening increases with group dispersion, i.e., the extent to which the group refractive index of the medium varies with wavelength and thickness of the tissue under investigation as well as with the spectral bandwidth of the light source. Measurements of the group dispersion in the cornea, lens and vitreous of pseudophakic and normal human eyes, show that the cornea and the lens are more dispersive than water-by a factor of about 5 and 2, respectively-in the investigated spectral region. The cornea is approximately threefold more dispersive than the human crystalline lens, the aqueous humor is less dispersive than water and the group dispersion of all ocular components together, averaged over the axial length of normal and pseudophakic eyes, was only slightly higher compared to that of water. Since the highly dispersive cornea and lens together have only a thickness of about one sixth of that of the axial eye length, it seems that their contribution to the group dispersive effect along the whole axial eye length is only small.
我们报告了使用双光束部分相干干涉测量法对水以及人眼介质(如角膜、房水、晶状体、人工晶状体)中的群折射率和群色散进行的定量测量,还给出了正常受试者和假晶状体患者在体情况下沿眼轴长度对这些介质进行平均后的总值。使用两个光谱位移光源展示了由于角膜色散导致的不同光学厚度值。该位移可用于间接计算人角膜在810纳米至860纳米光谱区域内的群色散。如果被研究对象具有色散性,由于检测信号的展宽,分辨率会受到限制。这种展宽随群色散增加,即介质的群折射率随被研究组织的波长、厚度以及光源的光谱带宽变化的程度。对假晶状体和正常人眼的角膜、晶状体和玻璃体中的群色散测量表明,在研究的光谱区域内,角膜和晶状体的色散性分别比水大约高5倍和2倍。角膜的色散性大约是人类晶状体的三倍,房水的色散性比水小,并且正常和假晶状体眼沿眼轴长度平均后的所有眼部成分的群色散仅比水略高。由于高色散的角膜和晶状体的总厚度仅约为眼轴长度的六分之一,因此它们对沿整个眼轴长度的群色散效应的贡献似乎很小。