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偏振对飞秒激光辐照LiF晶体的影响
引用本文:王承伟,赵全忠,张扬,王关德,钱静,鲍宗杰,李阳博,柏锋,范文中.偏振对飞秒激光辐照LiF晶体的影响[J].物理学报,2015,64(20):205204-205204.
作者姓名:王承伟  赵全忠  张扬  王关德  钱静  鲍宗杰  李阳博  柏锋  范文中
作者单位:1. 同济大学物理科学与工程学院, 上海 200092; 2. 中国科学院上海光学精密机械研究所, 强场激光物理国家重点实验室, 上海 201800; 3. 中国科学院大学, 北京 100049
基金项目:国家重点基础研究发展计划(批准号: 2011CB808103)和国家自然科学基金(批准号: 61178024, 11374316)资助的课题.
摘    要:飞秒激光聚焦到LiF晶体内部, 晶体的加工形貌随偏振改变. 实验表明, 偏振方向平行于<110> 晶向时, 加工起点到表面的距离是<100>偏振下的1.08 倍; 而<110>偏振下加工终点到表面的距离是<100> 偏振下的1.01 倍. 为了解释加工形貌的偏振依赖, 建立了逆韧致辐射、雪崩电离和无辐射跃迁的模型, 首先, 价带电子通过强场电离和雪崩电离, 从激光中吸收能量跃迁到导带, 该过程用电子密度演化方程和傍轴非线性薛定谔方程描述, 求解方程得到导带电子密度; 其次, 导带电子通过无辐射跃迁过程释放能量给晶格, 由能量守恒计算出晶格温度沿激光传播方向的分布; 最后, 晶格温度超过熔点以上的区域被加工. 模拟结果显示, <110>偏振下加工起点到表面的距离是<100> 偏振下的1.03倍, 而<110>偏振下加工终点到表面的距离是<100>偏振下的0.981 倍, 与实验结果基本一致. 虽然Z扫描技术测量的非线性折射率随偏振方向变化, 但是非线性折射率的变化趋势与实验结果相反. 模拟和实验证明逆韧致辐射导致加工形貌随偏振变化.

关 键 词:逆韧致辐射  无辐射跃迁  雪崩电离  非线性折射率
收稿时间:2015-03-16

Influence of polarization on irradiating LiF crystal by femtosecond laser
Wang Cheng-Wei,Zhao Quan-Zhong,Zhang Yang,Wang Guan-De,Qian Jing,Bao Zong-Jie,Li Yang-Bo,Bai Feng,Fan Wen-Zhong.Influence of polarization on irradiating LiF crystal by femtosecond laser[J].Acta Physica Sinica,2015,64(20):205204-205204.
Authors:Wang Cheng-Wei  Zhao Quan-Zhong  Zhang Yang  Wang Guan-De  Qian Jing  Bao Zong-Jie  Li Yang-Bo  Bai Feng  Fan Wen-Zhong
Institution:1. School of Physics Science and Engineering, Tongji University, Shanghai 200092, China; 2. State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China; 3. University of Chinese Academy of Sciences, Beijing 100049, China
Abstract:The processing morphology of cubic crystal LiF irradiated by femtosecond laser varies with the polarization direction. When the polarization direction is parallel to the crystal orientation <110>, the distance between the starting point and the surface is 1.08 times that along <100> polarization, and the distance between the end point and the surface is 1.01 times. While the cubic crystal is irradiated by a femtosecond laser, self-focusing and inverse bremsstrahlung are two probable mechanisms dependent on polarization. In order to investigate the relation between the self-focusing and polarization, in this paper we report the nonlinear refractive index n2 of LiF crystal which is linear with respect to selffocusing coefficient. The Z-scan technique is used to measure the nonlinear refractive indexes at different polarizations. As the polarization direction is rotated from <110> to <100>, the nonlinear refractive index decreases, and the self-focusing effect becomes weaker. If self-focusing leads to the dependence of morphology on polarization, the distance between the starting point and the surface for <100> polarization should be longer than that for <110> polarization. However, the experiment exhibits an opposite result that the distance between starting point and the surface for <100> polarization is shorter than that for <110> polarization. Therefore, the processing morphology which changes with polarization is not a consequence of the self-focusing. So in order to understand why the processing morphology varies with polarization, in this paper we present a model which combines inverse bremsstrahlung, avalanche ionization and radiationless transition. We believe that the recombination due to radiationless transition has a great effect on laser machining. The inverse bremsstrahlung coefficient of <110> polarization is less than that of <100> polarization, as a result, the density of free electrons which are produced by inverse bremsstrahlung and avalanche ionization at <110> polarization is less than that at <100> polarization. At first, the laser energy is transferred to the free electrons by inverse bremsstrahlung and avalanche ionization, which is described by the paraxial nonlinear Schrodinger equation and evolution equation of electron density. The density of free electrons is obtained by solving the equations. Then free electrons transfer the energy to the crystal lattice in the process of recombination through radiationless transition, which is depicted by energy conservation and gives the distribution of lattice temperature along the propagation direction. Finally, the area in LiF crystal of which the lattice temperature climbs up to above the melting point is processed. According to the simulation, the distance between the starting point and the surface at <110> polarization is 1.03 times that at <100> polarization, and the distance between the end point and the surface at <110> polarization is 0.981 times that at <100> polarization. These are consistent with the experimental results. Simulation and experimental results demonstrate that the inverse bremsstrahlung, which is dependent on polarization, is the main reason for morphology changing with the polarization of femtosecond laser. These research results may contribute to inducing microstructure in transparent dielectrics through femtosecond laser.
Keywords:inverse bremsstrahlung  radiationless transition  avalanche ionization  nonlinear refractive index
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