Hitzenberger C, Mengedoht K, Fercher A F
Fortschr Ophthalmol. 1989;86(2):159-61.
A new method has been developed for determining the axial length of the human eye. This method is based on laser interferometry with partially coherent light emitted by a multimode semiconductor laser diode. The measurement procedure is as follows. The subject looks into the laser beam (wavelength approximately equal to 780 nm, power approximately equal to 100 microW), which appears as a red spot. Hence the laser beam acts as a fixation target and measuring beam. This beam passes a Fabry-Perot interferometer in front of the eye. Reflected beams are generated at the cornea and retina. Since the coherence length of the laser used (approximately equal to 25 microns) is less than the difference in path length of the two reflected beams, they will usually not interfere with each other. However, if the distance between the interferometer plates is equal to the optical length of the eye, an interference pattern can be observed. (This is due to a second illuminating beam, which is generated by the interferometer and delayed by two times the interferometer plate distance.) During measurement, the plates are displaced relative to each other until the interference pattern is observed. At this point the plate distance, which can readily be measured, is equal to the optical eye length. This method has several advantages in comparison with the usual ultrasonic technique: it is a non-contact method; no anesthesia is needed; the optical eye length is determined directly; no assumptions need be made about sound velocities in the different eye media. High longitudinal and transversal resolution is achieved (10 microns or better possible). The first measurements obtained with the optical method were compared with the results yielded by the ultrasound technique.(ABSTRACT TRUNCATED AT 250 WORDS)
已开发出一种用于测定人眼眼轴长度的新方法。该方法基于多模半导体激光二极管发射的部分相干光的激光干涉测量法。测量过程如下。受试者注视激光束(波长约等于780纳米,功率约等于100微瓦),该激光束看起来是一个红点。因此,激光束既作为注视目标又作为测量光束。该光束穿过眼睛前方的法布里 - 珀罗干涉仪。在角膜和视网膜处产生反射光束。由于所用激光的相干长度(约等于25微米)小于两束反射光的光程差,它们通常不会相互干涉。然而,如果干涉仪平板之间的距离等于眼睛的光学长度,就可以观察到干涉图样。(这是由于干涉仪产生的第二束照明光束,其延迟了两倍的干涉仪平板距离。)在测量过程中,平板相对彼此移动,直到观察到干涉图样。此时,易于测量的平板距离就等于眼睛的光学长度。与常用的超声技术相比,该方法有几个优点:它是一种非接触式方法;无需麻醉;可直接测定眼睛的光学长度;无需对不同眼内介质中的声速做假设。可实现高纵向和横向分辨率(可达10微米或更好)。用光学方法获得的首批测量结果与超声技术得到的结果进行了比较。