低功率泵浦Ti：Al2O3自锁模激光器

本文报道了低功率泵浦的Ｔｉ：Ａｌ２Ｏ３激光器实现了稳定的自锁模运转，锁模脉冲宽度为１８０ｆｓ。分析了激光器的结构及工作特性。     

脉冲激光引起铜膜镜面的环形损伤波纹研究

用波长1.06μm、半高宽10ns的脉冲Nd:YAG激光辐照铜膜镜面,在激光辐照区,用光学显微镜观察到有规律的环形波纹状损伤图案,波纹平均周期约几十μm。通过对光路系统分析,认为样品前的小孔光阑对激光产生了菲涅尔衍射,使得在样品表面光强分布变成周期性环状分布。在极短的相互作用时间内,热扩散很小,损伤图案依赖于光强分布。并依据实验参数,用柯林斯公式对样品表面的光强分布进行了计算,所得光强分布的周期与损伤波纹的周期基本一致。     

短脉冲激光诱导薄膜损伤的等离子体爆炸过程分析

短脉冲激光诱导薄膜材料损伤过程的研究通常止于薄膜材料发生喷溅.超热喷溅物质吸收剩余激光脉冲能量将形成剧烈的等离子体爆炸过程.采用两步数值计算方法处理等离子体微滴的爆炸过程,即在每一个数值计算时间步长内,将爆炸过程分为两步,第一步处理微滴的绝热膨胀及裂解过程;第二步处理微滴对激光脉冲能量的吸收过程.有效地将微滴吸收激光能量的物理学过程与爆炸动力学过程耦合到一起.分析了喷溅物质微滴在剩余激光脉冲作用下,其半径、膨胀（加）速度、裂解（加）速度、电子及离子的密度与温度等参量随时间变化的演化情况.结果表明：材料喷溅 关键词： 光学薄膜 激光损伤 等离子体 爆炸     

ns脉冲激光对K9玻璃的破坏实验

采用高速PIN光电探测器和高带宽的数字存储示波器,实时检测透射光脉冲和散射光脉冲的变化特征,并将之用作材料破坏的光学判据,测量得到K9玻璃在1.06μm纳秒脉冲激光作用下的能量损伤阈值约18mJ,相应的能量密度阈值为1.0kJ/cm2。通过分析透射光脉冲和散射光脉冲的特征,给出了材料的破坏时刻,并推断出K9玻璃所能承受的极限光强为1015W/m2。研究了能量透过率与泵浦能量的关系,并初步探讨了透明材料的破坏机理。结果表明：在多纵模激光的作用下,透明光学材料破坏是电离击穿与自聚焦效应综合作用的结果。     

ns脉冲激光对K9玻璃的破坏实验

 采用高速PIN光电探测器和高带宽的数字存储示波器，实时检测透射光脉冲和散射光脉冲的变化特征，并将之用作材料破坏的光学判据，测量得到K9玻璃在1.06μm纳秒脉冲激光作用下的能量损伤阈值约18mJ，相应的能量密度阈值为1.0kJ/cm²。通过分析透射光脉冲和散射光脉冲的特征，给出了材料的破坏时刻，并推断出K9玻璃所能承受的极限光强为10¹⁵W/m²。研究了能量透过率与泵浦能量的关系，并初步探讨了透明材料的破坏机理。结果表明：在多纵模激光的作用下，透明光学材料破坏是电离击穿与自聚焦效应综合作用的结果。     

In-bulk and surface structuring of sapphire by femtosecond pulses

The actual space-time dependent intensity distribution of a tightly focused (numerical aperture NA = 1.35) Gaussian femtosecond pulse is modeled inside dielectric material. Such focusing is typically used for recording with sub-wavelength resolution inside dielectrics. The multi-pulse structuring inside the bulk and on the surface of sapphire are demonstrated. Formation of nano-cracks and nano-crystals is revealed inside the crystalline sapphire. Ripple formation on the surface is discussed in terms of the efficacy map calculated by theory given in ref. [J.E. Sipe, J.F. Young, J.S. Preston, H.M. van Driel, Laser-induced periodic surface structure. I. Theory, Phys. Rev. B 27 (2) (1983) 1141-1154.].     

Analysis of melt ejection during long pulsed laser drilling

In pulsed laser drilling, melt ejection greatly influences the keyhole shape and its quality as well, but its mechanism has not been well understood. In this paper, numerical simulation and experimental investigations based on 304 stainless steel and aluminum targets are performed to study the effects of material parameters on melt ejection. The numerical method is employed to predict the temperatures, velocity fields in the solid, liquid, and vapour front, and melt pool dynamics of targets as well. The experimental methods include the shadow-graphic technique, weight method, and optical microscope imaging, which are applied to real-time observations of melt ejection phenomena, measurements of collected melt and changes of target mass, observations of surface morphology and the cross-section of the keyhole, respectively. Numerical and experimental results show that the metallic material with high thermal diffusivity like aluminum is prone to have a thick liquid zone and a large quantity of melt ejection. Additionally, to the best of our knowledge, the liquid zone is used to illustrate the relations between melt ejection and material thermal diffusivity for the first time. The research result in this paper is useful for manufacturing optimization and quality control in laser-material interaction.     

多脉冲激光辐照下介质损伤理论研究

针对纳秒脉冲和飞秒脉冲不同的损伤机制,分别建立了两种多脉冲激光损伤模型。脉宽小于10 ps时,损伤是由于等离子体形成造成介质发生烧蚀所致,对此建立了基于电子密度演化方程的介质击穿模型;脉宽大于100 ps时,损伤是由于热沉积造成介质发生熔融所致,对此建立了基于傅里叶热传导方程的介质热损伤模型。通过计算两种模型下激光参数和材料参数对多脉冲损伤的影响,发现由于损伤机理不同,不同参数对单脉冲损伤阈值和多脉冲损伤阈值的影响趋势不完全一致,敏感程度也不同。通过计算得到了与实验结果一致的多脉冲损伤阈值与脉冲数间关系,使定量预估多脉冲损伤阈值和元件使用寿命成为可能。     

An experimental investigation of underwater pulsed laser forming

Laser forming is a new forming technology, which deforms a metal sheet using laser-induced thermal stresses. This paper presents an experimental investigation of pulsed laser forming of stainless steel in water and air. The effects of cooling conditions on bending angle and morphology of the heat affected zone (HAZ) are studied. It is shown that the case of the top surface in air and the bottom surface immersed in water has the greatest bending angle based on the forming mechanism of TGM. The water layer above the sample decreases the coupling energy, leading to a small bending angle. For a thin water thickness (1 mm), the water effects on the HAZ are limited. As water layer thickness increases (5 mm), the concave shape of the HAZ is more remarkable and irregular because the shock waves by high laser energy heating water are fully developed. However, the area and the depth of the HAZ become less significant when water thickness is 10 mm due to the long pathway that laser undergoes.     

Structural and optical properties of SrCu2O2 films deposited on sapphire substrates by pulsed laser deposition

We deposited SrCu₂O₂ (SCO) films on sapphire (Al₂O₃) (0 0 0 1) substrates by pulsed laser deposition. The crystallographic orientation of the SCO thin film showed clear dependence on the growth temperature. X-ray diffraction (XRD) and transmission electron microscopy (TEM) analysis showed that the film deposited at 400 °C was mainly oriented in the SCO [2 0 0] direction, whereas when the growth temperature was increased to 600 °C, the SCO film showed a dominant orientation of SCO [1 1 2]. The SCO film deposited at 500 °C was obvious polycrystalline, showing multi peaks from (2 0 0), (1 1 2), and (2 1 1) diffraction in the XRD spectrum. The SCO film deposited at 600 °C showed a band gap energy of 3.3 eV and transparency up to 80% around 500 nm. The photoluminescence (PL) spectra of the SCO films grown at 500 °C and 600 °C mainly showed blue-green emission, which was attributed to the intra-band transition of the isolated Cu⁺ and Cu⁺–Cu⁺ pairs according to the temperature dependent-PL analysis.     

钛合金纳秒激光打孔数值模拟和实验研究

为了描述纳秒激光对钛合金打孔过程中孔的形貌及温度场的变化规律,建立激光打孔的物理模型,利用ANSYS中APDL语言进行编程,对温度场进行仿真分析,并利用单元生死技术模拟孔形貌的变化过程。从有限元数值模拟和实验两方面综合分析比较了激光工艺参数(脉冲能量和脉冲数量)对打孔质量(孔深和孔径)的影响,系统论述了钛合金纳秒激光打孔的一般规律,以达到工艺参数优化,提高打孔质量的目的。     

激光散斑效应对激光雷达探测性能的影响

分析了激光散斑效应对激光雷达探测性能的影响. 给出了远场情况下接收物镜所采集激光散斑数的表达式. 在物镜所采集的散斑和光电子数均较大情况下，提出了光电子所遵守的分布. 分别导出了机载和星载激光雷达的探测概率. 分析表明激光雷达探测性能与所采集的散斑数密切相关，接收的散斑数仅与激光束腰和物镜的口径有关，随着接收散斑数的增加，散斑噪声的影响将减弱. 关键词： 激光雷达 激光散斑 探测概率     

An investigation into the effects of high laser fluence on hydroxyapatite/calcium phosphate films deposited by pulsed laser deposition

Pulsed laser deposited mixed hydroxyapatite (HA)/calcium phosphate thin films were prepared at room temperature using KrF laser source with different laser fluence varying between 2.4 J/cm² and 29.2 J/cm². Samples deposited at 2.4 J/cm² were partially amorphous and had rough surfaces with a lot of droplets while higher laser fluences showed higher level of crytallinity and lower roughness of surfaces of obtained samples. Higher laser fluences also decreased ratio Ca/P of as-deposited samples. X-ray photoelectron spectroscopy (XPS) revealed traces of carbonate groups in obtained samples, which were removed after thermal annealing. The decomposition of HA into TCP was observed to start at about 400 °C. The formation of new crystalline phase of HA was found after annealing as well. The cracks observed on surface of sample deposited at 29.2 J/cm² after annealing indicated that the HA/ calcium phosphate films deposited at higher laser energy densities were probably more densed.     

1064 nm纳秒激光对石墨烯的损伤效应研究

通过化学气相沉积法制备,并转移到基片得到1~3层石墨烯样品。利用霍尔效应及微区拉曼光谱测量,结合光学显微镜观察,分析了不同层数石墨烯在1064 nm纳秒激光辐照下的损伤特性。实验发现1~3层石墨烯的激光损伤阈值依次降低,分别为：单层0.45 J/cm2,2层0.34 J/cm2,3层0.23 J/cm2。激光强度超过阈值时,石墨烯薄膜电阻增大,载流子迁移率降低。通过光学显微镜观察发现局部区域破损,破损区域的拉曼光谱中1580 cm-1左右的G峰和2700 cm-1左右的2D峰高度比发生变化。实验结果表明1064 nm纳秒激光辐照石墨烯主要为剥离作用。     

CO2激光扫描辐照修复熔石英表面损伤

采用振镜系统结合10.6 m的CO2激光,对熔石英表面损伤点进行辐照,成功地修复了直径500 m的大尺寸损伤点,损伤修复后表面无烧蚀残留,损伤内部完全愈合,无气泡和残余裂纹。和定点修复方式相比,这种修复具有修复尺度大、面形影响区域小、应力分布范围小的优势。80%扫描辐照修复的损伤点的初始损伤阈值恢复甚至超过了基底的初始损伤阈值。     

An investigation into melt flow dynamics during repetitive pulsed laser drilling of transparent media

This paper presents an investigation into the dynamics of repetitive pulsed laser drilling of a visually transparent media using a CO₂ laser source. This enabled the use of a high-speed imaging system for observing, in real time, the behaviour of the drilling process in the laser drilled cavity of 1.5 mm diameter holes of up to 18.5 mm in depth. The work revealed that the instantaneous drilling velocity within each laser pulse can vary considerably from the average drilling velocity as a result of the non-uniform temporal pulse shape and the oscillation of the melt ejection rate. During beam breakthrough, both upward and downward melt ejections were observed to occur inside the drilled hole for a short period of time, after which the material was ejected through the exit end of the holes. It has been shown in this work that the downward melt flow velocity increases with hole depth for a positively tapered hole (from 0.09 to 1.43 m/s) and decreases with hole depth for a negatively tapered hole geometry (from 0.4 to 0.1 m/s), as a result of the change in the assist gas velocity inside the drilled hole with respect to the hole taper geometry. The mechanisms of forming the positively and negatively tapered holes in the transparent media have been correlated with the hole geometry and melt flow velocity. The work has demonstrated a new method of studying the melt dynamics in laser drilling.     

准分子激光诱导铅等离子体中谱线Stark展宽时空特性研究

测定了激光诱导铅等离子体中铅原子和离子谱线Ｓｔａｒｋ展宽的时间演化特性以及与缓冲气体压力之间的关系,由此计算得到了等离子体中电子密度的时间演化特性及其与缓冲气体压力之间的关系,实验结果表明,由不同的金属固体材料产生的激光等离子体的动力学性质差异很大,并讨论了形成这种差异的物理机制。     

多脉冲激光对K9玻璃的表面损伤实验研究

实验研究了波长为1 064 nm、脉宽为10 ns、重复频率为1 Hz的激光脉冲对K9玻璃的表面损伤特点,给出了脉冲透过能量随激光脉冲作用次数变化的规律。采用3维立体显微镜对损伤形貌进行观察,发现K9玻璃的损伤表面呈环状分布,分为烧蚀区、微裂纹区和断裂区。随着激光脉冲个数的增加,损伤由点状破坏演变为损伤区,微裂纹逐渐增长,损伤面积逐渐增大。基于激光支持的爆轰波理论分析,激光与脆性材料的相互作用可引起微裂纹的大量增长。在多脉冲激光的作用下,K9玻璃损伤的累积效应明显,表面损伤阈值明显降低,表面裂纹增长明显,损伤面积逐渐增大;但随着激光脉冲的继续增加,这种损伤趋于稳定。     

用散射光观察激光损伤的动态过程

本文利用散射光观察强激光对光学材料损伤的动态过程，详细说明了材料损伤时，散射光变化特点，以及损伤阈值的确定和散射光变化与损伤形貌的关系，并研究了激光损伤累积效应。     

无展宽器的高重复率钛宝石啁啾飞秒脉冲再生放大器的研究

通过优化放大腔结构参数和采用高光束质量的泵浦激光,依靠放大器腔内各个元件的色散展宽种子脉冲, 用钛宝石作为增益介质, 在低泵浦能量下, 实现了高光束质量,高稳定的中等能量的高重复率飞秒脉冲再生放大. 将钛宝石晶体离焦放置,有效的避免了光学损伤. 在1.1 mJ的绿光泵浦下, 获得了2 ps, 120 μJ, 重复频率为1 KHz, 光谱带宽7.8 nm的放大脉冲, 用石英棱镜对压缩可得到130 fs的激光脉冲.