1064nm与532nm激光对电子束蒸发制备的HfO2／SiO2高反膜损伤比较

研究了电子束蒸发制备的HfO2／SiO2高反膜在1064nm与532nm激光辐照下的损伤行为。基频激光辐照时损伤形貌主要为节瘤缺陷喷溅留下的锥形坑。当能量密度较大时出现分层剥落；二倍频激光损伤主要是由电子缺陷引起的平底坑，辐照脉冲能量密度稍高时也会产生吸收性缺陷引起的锥形坑，但电子缺陷的损伤阈值更低；随着辐照脉冲能量密度的增大分层剥落逐渐成为主要的损伤形貌。分析认为，辐照激光波长的变化。引起吸收机制的变化从而导致了损伤阈值及损伤机制的差异。

退火对HfO2/SiO2多层膜残余应力的影响

用电子束蒸发方法在BK7基底上沉积了HfO2/SiO2多层膜。研究了200℃到400℃的退火对残余应力的影响。结果表明退火前的薄膜残余应力为压应力，在200℃退火后发展为张应力，然后张应力值随着退火温度的升高而增大。在400℃退火后，由于张应力太大，薄膜表面出现了裂纹。同时，随着退火温度的升高，晶粒尺寸长大，晶面间距降低。残余应力的变化与结构的演变相对应。

HfO2的纯度对紫外多层膜反射率的影响

用辉光放电质谱法和二次离子质谱仪测定了两种HfO2材料及它们相应的单层膜中的杂质含量，结果发现，无论是在体材料中还是在用电子束蒸发技术沉积的材料单层薄膜中，ZrO2都是这两种HfO2材料中最主要的杂质。而且，这两种HfO2材料中Zr含量的差别远远大于Ti、Fe含量的差别，这说明Zr含量的差别正是引起两种HfO2膜层光学性能差别的原因。用这两种不同纯度的HfO2材料与同一纯度的SiO2材料组合，沉积形成266nm的紫外反射镜，实验结果表明这两种反射镜的反射率分别在99.85% 和 99.15%左右。这个结果与依据单层膜得出的光学常数所设计的结果符合的很好。

Influence of substoichiometer on the laser-induced damage characters of HfO2 thin films

HfO2 is one of the most important high refractive index materials for depositing high power optical mirrors. In this research, HfO2 thin films were prepared by dual-ion beam reactive sputtering method, and the laser-induced damage thresholds (LIDT) of the sample were measured in 1-on-1 mode for laser with 1064 nm wavelength. The results indicate that the LIDT of the as-grown sample is only 3.96 J/cm(2), but it is increased to 8.98 J/cm(2) after annealing under temperature of 200 degrees C in atmosphere. By measuring the laser weak absorption and SIMS of the samples, we deduced that substoichiometer is the main reason for the low LIDT of the as-grown sample, and the experiment results were well explained with the theory of electronic-avalanche ionization. (C) 2008 Elsevier B.V. All rights reserved.

Optimization of near-field optical field of multi-layer dielectric gratings for pulse compressor

Multi-layer dielectric (MLD) gratings for pulse compressors in high-energy laser systems should provide high diffraction efficiency as well as high laser induced damage thresholds (LIDT). Nonuniform optical near-field distribution is one of the important factors to limit their damage resistant capabilities. Electric field distributions in the gratings and multi-layer film region are analyzed by using Fourier modal method. Optimization of peak electric field in the gratings ridge is performed with a merit function, including both diffraction efficiency and electric field enhancement when the top layer material is HfO2 and SiO2, respectively. A set of optimized gratings parameters is obtained for each structure, which reduce the peak electric field within the gratings ridge to being respective 1.39 and 1.84 times the value of incident light respectively. Finally, we also discuss the effects of gratings refractive index, gratings sidewall angle and incident angle on peak electric field in the gratings ridge. (c) 2006 Elsevier B.V. All rights reserved.

单脉冲和多脉冲飞秒激光对单层光学薄膜的损伤

利用掺钛的蓝宝石飞秒激光系统输出的单脉冲和多脉冲飞秒激光（中心波长800nm，脉宽50fs,靶面聚焦直径Ф40／μm）。分别对BK7玻璃基底上厚约500nm的单层HfO2和单层ZrO2薄膜进行辐照,得到了这两种薄膜在1-on-1和1000-on-1测试方法下的激光损伤阙值。实验发现,两种方法下HfO2单层膜的阈值均比ZrO2单层膜的阈值高。从简化的Keldysh多光子离化理论出发，认为HfO2薄膜材料的带比ZrO2的宽是导致上述结果的主要原因。同时，同一种薄膜的多脉冲下的阙值比单脉冲下的低，原因是多脉冲下

多层介质膜光栅和介质膜反射镜抗激光损伤阈值研究

对多层介质膜光栅以及介质膜反射镜的激光损伤阈值进行了系统的研究。测试方法采用国际测试标准。测试结果表明，介质光栅的损伤阈值远低于未刻蚀的多层介质膜。对样品损伤形貌的扫描电镜照片分析发现，相比于未刻蚀的多层介质膜，介质膜光栅的初始损伤主要发生在光栅槽形的侧壁，且损伤主要是由驻波场的空间分布引起的本征吸收、制备过程中引入的杂质污染以及刻蚀过程中HfO2的化学计量机失衡引起的。

多层介质膜脉冲压缩光栅近场光学特性分析

利用傅里叶模式理论分析了TE波自准直角入射的使用条件下，多层介质膜光栅的光栅区和多层膜区电场分布的特点．分别讨论了HfO2和SiO2为顶层光栅材料时，光栅结构参数对光栅脊峰值电场的影响，结果表明，对于不同膜厚的顶层材料，存在一个最佳膜厚度，使光栅脊峰值电场最小，并且当膜厚增大时，设计大高宽比的光栅可以降低该电场峰值．最后，在大角度条件下使用多层膜光栅也可以降低光栅脊处的峰值电场．

多层介质膜脉宽压缩光栅的严格矢量分析

用于展宽和压缩激光脉冲的多层膜脉宽压缩光栅是由多层介质高反膜和位于其顶层的浮雕光栅构成。以设计的高反射多层膜为基础，利用傅里叶模式理论分析了其衍射场分布，给出了TE波自准直角入射的使用条件下，多层介质膜脉宽压缩光栅衍射效率的表达式。以-1级衍射效率为评价函数，分别讨论了HfO2和SiO2为顶层材料时，多层膜脉宽压缩光栅-1级衍射效率高于0．95的光栅结构参量范围。结果表明，在该条件下，选择HfO2为顶层材料时，光栅结构参量有较大的取值范围。给出了优化的光栅结构参量，并分析了光栅制作误差及其使用条件的宽容度