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1.
利用Nd∶YAG调Q单脉冲激光和自由脉冲激光对硬膜窄带干涉滤光片进行激光损伤阈值的测试,并且采用表面热透镜技术测量了滤光片的吸收率。实验发现:窄带干涉滤光片的吸收率和激光损伤阈值强烈依赖于辐照激光波长与窄带干涉滤光片通带的相对位置;在调Q单脉冲激光作用下,不同中心波长的滤光片损伤形貌存在明显的差别,而在自由脉冲激光作用下,各滤光片的损伤形貌则趋于相同,均表现为典型的热熔烧蚀破坏。根据实验结果,结合损伤形貌,通过驻波场理论对激光作用下滤光片内电场分布的分析与模拟,探讨了两种激光模式作用下滤光片的损伤特征和损伤机理的不同特点。  相似文献   

2.
The laser-induced damage behavior of narrow-band interference filters was investigated with a Nd:YAG laser at 1064 nm under single-pulse mode and free-running laser mode.The absorption measurement of such coatings has been performed by surface thermal lensing(STL)technique.The relationship between damage morphology and absorption under the two different laser modes was studied in detail.The explanation was given by the standing-wave distribution theory.  相似文献   

3.
Zirconium dioxide (ZrO2) thin films were deposited on BK7 glass substrates by the electron beam evaporation method. A continuous wave CO2 laser was used to anneal the ZrO2 thin films to investigate whether beneficial changes could be produced. After annealing at different laser scanning speeds by CO2 laser, weak absorption of the coatings was measured by the surface thermal lensing (STL) technique, and then laser-induced damage threshold (LIDT) was also determined. It was found that the weak absorption decreased first, while the laser scanning speed is below some value, then increased. The LIDT of the ZrO2 coatings decreased greatly when the laser scanning speeds were below some value. A Nomarski microscope was employed to map the damage morphology, and it was found that the damage behavior was defect-initiated both for annealed and as-deposited samples. The influences of post-deposition CO2 laser annealing on the structural and mechanical properties of the films have also been investigated by X-ray diffraction and ZYGO interferometer. It was found that the microstructure of the ZrO2 films did not change. The residual stress in ZrO2 films showed a tendency from tensile to compressive after CO2 laser annealing, and the variation quantity of the residual stress increased with decreasing laser scanning speed. The residual stress may be mitigated to some extent at proper treatment parameters.  相似文献   

4.
TiO2 single layers and TiO2/SiO2 high reflectors (HR) are prepared by electron beam evaporation at different TiO2 deposition rates. It is found that the changes of properties of TiO2 films with the increase of rate, such as the increase of refractive index and extinction coefficient and the decrease of physical thickness, lead to the spectrum shift and reflectivity bandwidth broadening of HR together with the increase of absorption and decrease of laser-induced damage threshold. The damages are found of different morphologies: a shallow pit to a seriously delaminated and deep crater, and the different amorphous-to-anatase-to-rutile phase transition processes detected by Raman study. The frequency shift of Raman vibration mode correlates with the strain in film. Energy dispersive X-ray analysis reveals that impurities and non-stoichiometric defects are two absorption initiations resulting to the laser-induced transformation.  相似文献   

5.
High reflectivity coating is designed and fabricated with HfO2/SiO2 stacks. The laser-induced damage experiment is prepared by a third-order harmonic generation of Nd:YAG laser (355 nm, 8 ns). Typical damage micrographs are obtained using atomic force microscope (AFM) and scanning electron microscope (SEM). A theoretical model based on the thermal transfer is tried to describe the defect dependence of damage morphology. Three situations are considered in this model: single defect, couple defects and high absorption film. The calculated results show that the second situation agrees well with the experiment.  相似文献   

6.
The effects of annealing on structure and laser-induced damage threshold (LIDT) of Ta2O5/SiO2 dielectric mirrors were investigated. Ta2O5/SiO2 multilayer was prepared by ion beam sputtering (IBS), then annealed in air under the temperature from 100 to 400 °C. Microstructure of the samples was characterized by X-ray diffraction (XRD). Absorption of the multilayer was measured by surface thermal lensing (STL) technique. The laser-induced damage threshold was assessed using 1064 nm free pulsed laser at a pulse length of 220 μs.

It was found that the center wavelength shifted to long wavelength gradually as the annealing temperature increased, and kept its non-crystalline structure even after annealing. The absorbance of the reflectors decreased after annealing. A remarkable increase of the laser-induced damage threshold was found when the annealing temperature was above 250 °C.  相似文献   


7.
铜膜和铁膜污染物诱导熔石英表面损伤行为的对比研究   总被引:1,自引:0,他引:1  
采用人工溅射的方式分别在熔石英基片上镀制了光学厚度相近的铜膜和铁膜污染物。研究了熔石英基底在355nm波长的激光损伤阈值。分别采用透射式光热透镜技术、椭偏仪、原子力显微镜和光学显微镜研究了两类薄膜的热吸收、膜层厚度、表面微观形貌以及激光辐照后薄膜的损伤形貌。实验结果表明:熔石英表面的金属膜状污染物均导致基片损伤阈值下降,位于前表面的污染物引起的损伤阈值下降更为严重,约为23%。两种污染物薄膜引起基底的损伤形貌、基底损伤阈值的下降幅度与薄膜的热吸收系数与微观结构有关。从热力学响应角度,结合损伤形貌对污染物诱导熔石英表面形貌的损伤机理进行了讨论。  相似文献   

8.
HfO2/SiO2高反射膜的缺陷及其激光损伤   总被引:14,自引:10,他引:4       下载免费PDF全文
用原子力、Normaski和扫描电子显微镜等分析仪器,对高损伤阈值薄膜常采用HfO2/SiO2薄膜进行了表面显微图象研究,分析了薄膜常见的表面缺陷,如节瘤,孔洞和划痕等。薄膜表面缺陷的激光损伤实验表明,不同缺陷的抗激光损伤能力不大相同。节瘤缺陷最低,约为15J/cm^2,薄膜的损伤阈值主要由其决定,孔洞的激光损伤能力与节瘤相比较高,约为节瘤的2-3倍。节瘤缺陷在低能量密度的激光损伤所形成的孔洞,与镀制过程中形成的孔洞形貌相似,激光再损伤能力也相似。低能量密度的激光把瘤缺陷变为孔洞缺陷是激光预处理提高薄膜损伤阈值的原因之一。  相似文献   

9.
在低于一个标准大气压的条件下对飞秒激光产生的N2等离子体光谱进行了实验研究.结果表明, 各种样品气压下的激光N2等离子体光谱均表现为连续谱和线状谱的叠加.随着样品气压的降低, 连续谱和原子谱线的强度经历了由缓慢增强发展为缓慢降低再到迅速降低的过程, 而正一价离子谱线强度呈现逐步增强的特征.在气压低于0.3 atm (1 atm=101325 Pa)时, 出现了正二价态的离子谱线. 给出了低压N2等离子体对于飞秒激光传输和能量吸收的物理特性, 并初步讨论了低压等离子体通道特性.这些结果有助于加深了解飞秒激光等离子体的特性和机理, 特别是给出了在实验上测量不同价态离子光谱的条件, 为今后的研究提供了有益的实验依据. 关键词: 飞秒激光 气压 等离子体光谱 激光传输  相似文献   

10.
激光预处理是提高激光薄膜抗激光损伤阈值的重要手段。对电子束蒸发方式镀制的HfO2/SiO2反射膜采用大口径激光进行了辐照,并采用激光量热计测量了激光辐射前后的弱吸收值。采用聚焦离子束(FIB)技术分析了激光辐照后薄膜的损伤形态并探究了损伤原因,首次采用扫描电镜拍摄到了节瘤部分喷发时的形貌图,并对其进行了FIB分析,为进一步了解节瘤的损伤过程提供了依据。实验发现,激光辐照过后的激光薄膜弱吸收明显降低,激光预处理有效减少了引起薄膜吸收的缺陷,存在明显的清洗效应;在本实验采用的HfO2/SiO2反射膜中,激光预处理技术对于祛除位于基底上种子形成的节瘤是有效的,原因是激光辐射过后该节瘤进行了预喷发并不会对后续激光产生影响;而激光预处理技术对位于膜层中间的可能是镀膜过程中材料飞溅引起的缺陷是无效的,需要通过其他手段对该类节瘤进行祛除。  相似文献   

11.
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/cm2, but it is increased to 8.98 J/cm2 after annealing under temperature of 200 °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.  相似文献   

12.
为了了解采用脉冲CO2激光推进空气呼吸模式时光船参数等对产生等离子体的影响,介绍了利用实验室自行研制的紫外预电离TEA CO2激光器进行的激光等离子体实验。实验采用底面直径为60mm、焦距为5mm和10mm的抛物面光船。介绍了空气呼吸模式激光等离子体的谱和明显的特征谱线,以及等离子体的时间演化过程。结果表明:空气呼吸模式等离子体的持续时间约为20μs,在6μs左右时信号强度达到最大值;激光脉冲作用后,信号迅速衰减;10mm光船产生的等离子体信号峰值和持续时间均略长于5mm光船的。  相似文献   

13.
 研究了SiO2半波覆盖层对HfO2/SiO2高反射膜1064nm激光损伤的影响,分析薄膜的激光损伤特性及图貌得出, 对于单脉冲(1-ON-1)激光损伤,SiO2半波覆盖层能提高HfO2/SiO2高反膜的激光损伤阈值;可显著降低激光损伤程度,减小灾难性损伤发生的概率;可大幅度提高HfO2/SiO2高反膜膜的抗激光损伤能力。  相似文献   

14.
 分别采用电子束热蒸发技术和溶胶-凝胶技术在K9基片上镀制了光学厚度相近的ZrO2单层薄膜,测试了两类薄膜的激光损伤阈值。分别采用透射式光热透镜技术、椭偏仪、原子力显微镜和光学显微镜研究了两类薄膜的热吸收、孔隙率、微观表面形貌、激光辐照前薄膜的杂质和缺陷状况以及激光辐照后薄膜的损伤形貌。实验结果表明:两类薄膜的不同损伤形貌与薄膜的热吸收与微观结构有关, 物理法制备的ZrO2膜结构致密紧凑,膜层的杂质和缺陷多;化学法制备的ZrO2膜结构疏松多孔,膜层纯净杂质少,激光损伤阈值达26.9 J/cm2;因物理法制备的ZrO2膜拥有更大的热吸收(115.10×10-6)和更小的孔隙率(0.20),其激光损伤阈值较小(18.8 J/cm2),损伤主要为溅射和应力破坏,而化学法制备的ZrO2膜的损伤主要为剥层。理论上对实验结果进行了解释。  相似文献   

15.
采用单台阶能量光栅扫描以及R-on-1测试两种不同预处理方式研究了激光预处理技术对532nm HfO2/SiO2高反膜的阈值提升效果。用Nd:YAG二倍频激光对电子束蒸发制备的532nm HfO2/SiO2高反膜进行1-on-1损伤阈值测试,然后分别进行单台阶能量光栅扫描以及R-on-1测试。通过对损伤概率以及损伤形貌的分析,发现激光预处理能够去除薄膜内低阈值缺陷,达到提高损伤阈值的目的,损伤阈值分别提高38%和30%。  相似文献   

16.
根据已建立的理论模型,计算得到了K9玻璃受脉冲CO_2激光辐照时产生的热应力分布,研究了热应力的时间特征,在分析样品尺寸对损伤结果影响的基础上,提出了K9玻璃抗激光损伤的最佳半径。结果表明:K9玻璃产生的热应力损伤主要由环向应力控制,热应力以热冲击波的形式在样品内传播,大小随时间变化而来回振荡,且激光脉冲结束后比激光作用时间内产生的热应力要大。这说明若样品在激光加热期间产生的热应力不足以造成材料破坏,则有可能会在其后的冷却过程中产生更大的热应力,材料将会在冷却过程中发生破裂。根据样品参数对损伤结果的影响,进一步验证了K9玻璃抗激光损伤最佳半径的通用性。  相似文献   

17.
Ta2O5 and Nb2O5 films are deposited on BK7 glass substrates using an electron beam evaporation method and are annealed at 673 K in the air.In this letter,comparative studies of the optical transmittance,microstructure,chemical composition,optical absorption,and laser-induced damage threshold(LIDT) of the two films are conducted.Findings indicate that the substoichiometric defect is very harmful to the laser damage resistance of Ta2O5 and Nb2O5 films.The decrease of absorption improves the LIDT in films deposited by the same material.However,although the absorption of the Ta2O5 single layer is less than that of the Nb2O5 single layer,the LIDT of the former is lower than that of the latter.High-reflective(HR) coatings have a higher LIDT than single layers due to the thermal dissipation of the SiO2 layers and the decreased electric field intensity(EFI).In addition,the Nb2O5 HR coating achieves the highest LIDT at 25.6 J/cm 2 in both single layers and HR coatings.  相似文献   

18.
Laser-induced damage is associated with nodular defects in HfO2/SiO2 multilayer films. In order to investigate the damage characteristics of HfO2/SiO2 multilayer mirrors and find the information of improving laser-induced damage threshold, nodular defects are characterized by multiple analytical techniques; the damage morphologies induced by nodular-ejections are presented; the depths of nodular-ejection pits are investigated; the laser-induced damage threshold of zero probability and the stabilities of nodular-ejection pits exposed to repetitive illuminations are studied. Results show that domes in the film surface are nodular defects. Reliable depth information of nodular-ejection pits is obtained by counting layers from the damage edge. The depth statistical result implies nodular defects in these samples are usually originated from deep seeds. Some process optimizations suggestions are given based on the depth information. A simple tractable method is proposed to determine the functional damage threshold of these HfO2/SiO2 multilayer films basing on the damage experiments.  相似文献   

19.
采用溶胶-凝胶方法制备了ZrO2-TiO2(Ti含量为0—100mol%)高折射率光学薄膜. 借助激光动态光散射技术研究溶胶微结构. 采用傅里叶变换红外光谱、原子力显微镜、薄膜光学常数分析仪、漫反射吸收光谱及强激光辐照实验,对膜层的结构、光学性能及抗激光损伤性能进行了系统表征. 结果显示,溶胶-凝胶工艺可以在部分牺牲折射率的情况下,使膜层的抗激光损伤性能得到大幅度提升. 随Ti含量从0mol%增加至100mol%,膜层的平均损伤阈值呈下降趋势,当Ti含量从0mol%增加至60mol%时,平均损伤阈值从57.1J/cm2下降到21.1J/cm2(辐照激光波长为1053nm,脉冲宽度为10ns,“R/1”测试模式),当Ti含量从60mol%增加至100mol%时,平均损伤阈值变化很小. 综合溶胶微结构、膜层光学性能和损伤实验结果可以推断,强激光诱导多光子吸收是引起膜层损伤的主要原因. 不同配比的复合膜之间光学带隙的显著差异导致相同辐照激光情况下多光子吸收的概率发生变化,从而导致损伤阈值的规律性变化. 关键词: 2-TiO2薄膜')" href="#">ZrO2-TiO2薄膜 溶胶-凝胶 激光诱导损伤 光学带隙  相似文献   

20.
研究了CO2激光局域辐照对熔石英损伤特性的影响, 发现当辐照中心温度较低时(1139 K), 辐照对损伤阈值没有明显影响, 但辐照中心温度较高时(1638 K), 辐照对损伤阈值有明显的影响, 损伤阈值随距离辐照中心间距的增大而减小, 在残余应力产生光程差最大处附近, 损伤阈值降到最小, 随着与辐照中心间距的进一步增加, 损伤阈值略有上升. 对导致此现象的原因做了分析. 由于残余应力的存在, 在辐照中心发生再损伤产生的裂纹后, 裂纹先沿径向扩展, 在残余应力产生光程差最大处附近, 裂纹转而向切向扩展, 这可能与径向和环向张应力随半径的变化有关. 在采用热处理炉退火消除残余应力时, 必须注意元件的洁净处理, 否则退火会出现析晶现象, 对损伤阈值和透射率造成不良影响. 关键词: 2激光局域辐照')" href="#">CO2激光局域辐照 熔石英 损伤特性  相似文献   

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