自由电子激光在2.7 ~ 6.7微米范围内光烧蚀明胶。

B. Jean, T. Bende
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引用次数: 8

摘要

背景:红外光消融是未来屈光手术和角膜手术的一种选择;其基本原理尚未得到系统的研究。第一次,自由电子激光器允许在宽波长范围内,以可变的脉冲长度和能量组合进行光烧蚀的动态研究。本研究的目的是利用自由电子激光作为定量描述红外光烧蚀的工具。我们研究了波长的函数,因为它与目标材料光谱、角膜水化和脉冲重复率的影响有关。方法在2.7 ~ 6.7微米范围内对人角膜和明胶进行表面吸收光谱分析。明确厚度(140 +/- 5微米)和控制水合作用(湿/干重1至4.5)的明胶探针作为目标材料。1992年9月,使用范德比尔特大学自由电子激光器(田纳西州纳什维尔)进行光消融,影响为1.27 J/cm2, 4微秒的大脉冲,由2 ps微脉冲组成,脉冲重复率为2.9 GHz。在稳定的光束轮廓下,波长在2.7和6.7微米之间可调。消融实验作为能量、水合作用和脉冲重复率的函数进行。通过a)穿孔实验和b)共聚焦激光地形测量法(UBM, Ettlingen, FRG)直接测量来评估消融率。结果通过穿孔实验和地形测量评估的消融速率与目标材料相应的吸光度具有良好的相关性:在3微米和6微米吸水带附近,最大目标吸光度处的最大消融速率。6.2微米处的烧蚀阈值为0.7 +/- 0.05 J/cm2(穿孔),深度测量值为0.55 +/- 0.08 J/cm2。消融率作为水合作用的函数增加到2.3(湿/干重),水合作用越高,消融率越低。消融率作为脉冲重复率的函数显示高达20 Hz的增加,在那里它被发现高出60%。结论自由电子激光技术的首次系统应用将烧蚀效率与目标材料的吸收呈正相关,从而为角膜组织等高含水量材料确定了一个“新的”有前途的波长,约为6.2微米。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Photoablation of gelatin with the free-electron laser between 2.7 and 6.7 microns.
BACKGROUND Photoablation in the infrared (IR) is an option for future refractive and corneal surgery; its basic principles have not yet been investigated systematically. For the first time, the free electron laser allows the dynamic study of photoablation over a wide range of wavelengths with variable combinations of pulselength and energy. The goal of this study is to use the free electron laser as a tool to describe photoablation in the IR quantitatively. We studied the function of wavelength as it is related to target material spectroscopy and the effects of corneal hydration and the pulse repetition rate. METHODS Surface absorption spectroscopy of the human cornea and of gelatin as a proven model of the cornea was performed between 2.7 and 6.7 microns. Gelatin probes of well-defined thickness (140 +/- 5 microns) and controlled hydration (wet/dry weight 1 to 4.5) served as target material. Photoablation was performed with the Vanderbilt University free electron laser (Nashville, Tenn) in September 1992 at a fluence of 1.27 J/cm2, and a macropulse of 4 microseconds, composed of 2 ps micropulses at a 2.9 GHz pulse repetition rate. Wavelength was tunable between 2.7 and 6.7 microns at stable beam profiles. Ablation experiments were performed as a function of energy, hydration, and pulse repetition rate. Ablation rates were assessed by a) perforation experiments, and b) direct measurements using confocal laser topometry (UBM, Ettlingen, FRG). RESULTS Ablation rate, assessed by perforation experiments and topometry, correlated well with the corresponding measured absorbencies of the target material: maximal ablation rate at maximal target absorption, around the 3- and 6-micrometer water absorption bands. The ablation threshold at 6.2 microns was 0.7 +/- 0.05 J/cm2 (perforation) and 0.55 +/- 0.08 J/cm2 for depth measurements. Ablation rate as a function of hydration increased to 2.3 (wet/dry weight) with a decrease for higher hydrations. Ablation rate as a function of the pulse repetition rate showed an increase of up to 20 Hz, where it was found to be 60% higher. CONCLUSION The first systematic use of free electron laser technology positively correlated ablation efficiency with target material absorption, thus identifying a "new" promising wavelength at around 6.2 microns for materials with a high water content such as corneal tissue.
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