强流脉冲电子束表面改性的物理模型及数值模拟

 推导出了强流脉冲电子束处理过程的应力场方程，利用数值模拟，得到了温度场和应力场的分布曲线，分别给出了熔化深度、升降温的速率及温度梯度的大小，准静态应力和热应力波的幅值、应力波的传播及反射过程，利用数值模拟结果对实验中观察到的实验现象熔化深度、材料表层及次表层数微米范围内组织结构的变化及数百微米的硬度提高等给出了解释。     

强脉冲电子束辐照材料表面形貌演化的模拟

在回顾和总结强脉冲电子束表面改性实验的基础上, 利用有限元数值计算方法对强脉冲电子束辐照铝和304不锈钢产生的温度场进行模拟, 给出了靶的近表面区域流体状态存在的特征尺度和特征时间, 并对不同材料特性下熔坑的产生原因进行了讨论. 采用两相流模型, 通过水平集方法和有限元方法结合的计算流体力学模拟了熔坑和表面突起形貌在表面处于熔融状态下的运动特征, 通过和实验数据相对比, 验证了对于高黏度, 高表面张力的高熔点金属, 表面处于流体状态下的张力驱动效应是熔坑等表面形貌演化的重要原因.     

飞秒激光辐照铝靶产生快电子发射的实验和模拟研究

采用实验和数值模拟研究了飞秒激光辐照铝靶产生的快电子发射.实验中,在主脉冲前加上一个预脉冲产生预等离子体,然后主脉冲与预等离子体作用产生快电子.在激光反射方向附近,实验测量的快电子束发射与数值模拟的结果高度地一致;在靶背面,发射的快电子的数目小于数值模拟的结果,原因在于快电子在靶内输运受到电荷分离场和碰撞的影响;在数值模拟中未出现的,沿靶表面发射的快电子束,是由表面准静态电磁场的禁闭效应产生.     

飞秒激光辐照铝靶产生快电子发射的实验和模拟研究

采用实验和数值模拟研究了飞秒激光辐照铝靶产生的快电子发射。实验中，在主脉冲前加上一个预脉冲产生预等离子体，然后主脉冲与预等离子体作用产生快电子。在激光反射方向附近，实验测量的快电子束发射与数值模拟的结果高度地一致；在靶背面，发射的快电子的数目小于数值模拟的结果，原因在于快电子在靶内输运受到电荷分离场和碰撞的影响；在数值模拟中未出现的，沿靶表面发射的快电子束，是由表面准静态电磁场的禁闭效应产生。     

强流脉冲电子束应力诱发的微观结构

利用强流脉冲电子束装置在各种工艺条件下对奥氏体不锈钢、单晶铝及多晶铝等面心立方金属进行辐照处理.利用扫描电子显微镜和透射电子显微镜等详细分析了辐照样品的变形组织与结构.通过分析，在一定程度上建立起强流脉冲电子束诱发的应力特征与变形结构之间的关系，并对目前现有的几种应力波数值模拟结果进行了分析.实验结果表明，强流脉冲电子束能够在材料内部诱发10²—10³MPa的应力，其传播方式与材料的 晶体结构关系密切.这一应力是导致材料深层性能与微观组织结构发生变化的根源所在. 关键词： 强流脉冲电子束 应力 微观结构 变形     

强流脉冲电子束作用下纯镍表面的应力特征

 利用强流脉冲电子束（HCPEB）装置对多晶纯镍进行轰击,采用X射线衍射及扫描电子显微镜等技术,详细分析了受轰击样品的变形组织与结构。通过分析建立了强流脉冲电子束诱发的应力特征与变形结构之间的关系,并对目前现有的几种应力波数值模拟结果进行了讨论。实验结果表明：强流脉冲电子束能够在材料表层诱发约5GPa的应力,造成纯镍表面发生孪生塑性变形。除了热膨胀引起的表层横向准静态热应力外,强流脉冲电子束产生的等离子体脉冲爆炸可以直接诱发幅值很高的冲击应力波,二者的共同作用是引起表层微观结构变化的直接原因。     

强流脉冲电子束辐照下单晶铝中的堆垛层错四面体

利用强流脉冲电子束技术对单晶铝进行了辐照，并利用透射电镜对强流脉冲电子束诱发的空位簇缺陷进行分析.实验结果表明，强流脉冲电子束能够诱发位错圈、孔洞甚至堆垛层错四面体这种通常在高层错能金属中不能形成的空位簇缺陷，并且三种不同类型的空位簇缺陷的形核过程并不同时发生，三种空位簇缺陷存在着密切的关系.根据实验结果提出了堆垛层错四面体形成与生长机理. 关键词： 强流脉冲电子束 堆垛层错四面体 单晶铝 空位簇缺陷     

RAFM钢TIG焊和电子束焊疲劳性能实验和分析模拟

利用ANSYS 对低活化铁素体马氏体(RAFM)钢进行非熔化极气体保护焊(TIG 焊)与电子束焊的抗疲劳模拟分析，再利用SDS200 电液伺服疲劳试验机对TIG 焊和电子束焊的两种RAFM 钢试件进行实验。通过施加相同梯度负荷对TIG 焊和电子束焊试件进行焊缝的疲劳性能实验。与实验结果对比分析，结果显示电子束焊优于 TIG 焊，但在一定负载下可以用TIG 焊代替电子束焊。     

强流脉冲电子束诱发纯镍表层纳米结构的形成机制

利用强流脉冲电子束（HCPEB）技术对多晶纯镍进行了表面处理,并采用扫描电镜和透射电镜对强流脉冲电子束诱发的表面及亚表面的微观组织结构进行了分析.实验结果表明,HCPEB辐照后表面熔化,形成了深度约为2 μm的重熔层,快速的凝固使重熔层中形成晶粒尺寸约为80 nm的纳米结构.位于轰击表面下方5—15 μm深度范围内强烈塑性变形引起的位错墙和其内部的亚位错墙结构是该区域的主要结构特征.这些缺陷结构通过互相交割细化晶粒,最终导致尺寸约为10 nm的纳米晶粒的形成. 关键词： 强流脉冲电子束 纳米结构 多晶纯镍 位错墙     

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通过电子束辐照实验和有限元模拟研究了ITER类型面对等离子体的高纯钨材料在瞬态热冲击下的行为。在新建成的电子束实验平台EMS-60上进行了ITER等离子体发生大破裂不稳定下的模拟实验,实验中样品的基体温度为室温,脉冲宽度为1-5ms,能量负载范围是1~5MJ-m-2。实验后通过扫描电镜观察了样品的再结晶、裂纹及熔化情况,讨论了裂纹形成机理。通过有限元模拟,得出在5ms的脉冲负载下钨的裂纹阈值为1.5MJ-m-2,与实验结果符合很好。     

Phase explosion induced by high-repetition rate pulsed laser

The characteristics and mechanisms of the damage to absorbing glass with high-repetition laser pulses (several kHz) are discussed. The results show that: (1) in the range of comparatively low-repetition rate, the damage is characterized by material melting and a small crater on the surface of substrate; (2) with the increase in repetition rate, a bigger and deeper crater is surrounded by re-deposition and crystalline granules originating from the cooling of vapor; and (3) the crater, surrounded by evaporation and an large number of solid particulates which is obviously the characters of phase explosion, becomes even bigger and deeper when the repetition rate is further increased. We modeled the temperature distribution in different repetition rate regime and found that heat accumulation plays a significant role in damage process. Because of the temperature dependence of damage mechanism, the temperature of the area irradiated by laser beam will ramp up with increasing the repetition rate, which triggers the melting and evaporation of dielectrics and phase explosion successively. Our results may benefit the understanding of laser-induced damage in optical materials.     

Irradiation effects of CO2 laser parameters on surface morphology of fused silica

To understand the surface morphology evolution of fused silica induced by 10.6-μm CO2 laser irradiation at different parameters,this paper reports that optical microscopy,profilometry,and hydrophilicity tests are utilized to characterize the surface structure and roughness of the laser irradiated area. The results show that three typical surface morphologies and two typical hydrophilicity test images are observed at different laser powers and pulse durations. The correlations between surface temperature and surface morphology as well as hydrophilicity behaviours are presented. The different hydrophilicity behaviours are related to surface structures of the laser-induced crater and thermal diffusion area. The thermal diffusion length monotonously increases with increasing laser power and pulse duration. The crater width is almost determined by the laser beam size. The crater depth is more sensitive to the laser power and pulse duration than the crater width.     

高重复频率激光脉冲光束大小对吸收玻璃损伤特征的影响

针对高重复频率对吸收性滤光片损伤问题,研究了高重复频率(kHz量级)激光脉冲的光束半径大小对吸收玻璃的形貌特征和损伤机理.研究发现在总的激光作用个数、单脉冲能量和脉冲作用频率固定时,吸收玻璃的损伤特性发生很大变化:在光束半径较大时,激光能量分散,主要损伤形貌是熔化破坏;随着光束半径的减小,激光脉冲能量变得集中,热量的累积效果变得明显,逐渐变成熔化破坏和气化破坏;当激光光束半径小到一定程度,则会由于光强过大使得介质表面发生击穿而产生激光等离子体冲击波,同时由于热量沉积的集中使光束作用中心处产生超热液体,当满足相爆炸发生的条件时,气化物、液滴和固体颗粒的混合物会向外飞溅,在损伤凹陷的周围形成气化物、液滴的冷凝区和固体颗粒溅射区. 关键词： 激光诱导损伤 高重复激光脉冲 吸收玻璃 相爆炸     

三倍频分光膜在1064 nm的破斑特性研究

采用电子束蒸发方式制备了两种不同材料组合的分光膜,分别对其在波长1064 nm激光辐照下的损伤阈值进行了测试,用Alpha-Step 500台阶仪对破斑进行了深度测量。实验结果表明,破斑呈现出表面层的剥落和深坑破坏两种形态。表面层的剥落深度在一定范围内不随能量密度的变化而变化;深坑破坏深浅不一,是膜内缺陷融化、汽化及喷发的综合作用的结果,是损伤阈值降低的主要原因。     

Theoretical study of the influence of laser-induced defects on the adsorption of gases on solid surfaces

Laser treatment of a solid surface was modeled by applying an analytical theory as well as by using Monte Carlo simulations. The crystalline surface was assumed to be initially smooth and chemically uniform, that is free of impurities built into the structure. Creation of surface defects by a laser beam was assumed to have entirely random nature. In particular, the surface was assumed to have been scanned by the beam focused successively on randomly chosen points. In the course of the ablation process, the beam produces a pyramidal crater whose dimensions are proportional to the applied laser power. According to the assumed nature of the scanning procedure, the craters formed by the beam are allowed to overlap. The influence of the number of laser pulses and the crater dimensions on the structural and adsorptive properties of the surface were examined by analysis of the variation of the mean surface depth and the surface width. Changes in the adsorptive properties were also estimated by the calculation of the thermally programmed desorption (TPD) spectra of monomolecular adsorbates desorbed from laser-treated surfaces. Additionally, equilibrium adsorption isotherms were calculated for the obtained surfaces.     

Thermal affected zone obtained in machining steel XC42 by high-power continuous CO2 laser

A high-power continuous CO₂ laser (4 kW) can provide energy capable of causing melting or even, with a special treatment of the surface, vaporization of an XC42-steel sample. The laser–metal interaction causes an energetic machining mechanism, which takes place according to the assumption that the melting front precedes the laser beam, such that the laser beam interacts with a preheated surface whose temperature is near the melting point. The proposed model, obtained from the energy balance during the interaction time, concerns the case of machining with an inert gas jet and permits the calculation of the characteristic parameters of the groove according to the characteristic laser parameters (absorbed laser energy and impact diameter of the laser beam) and allows the estimation of the quantity of the energy causing the thermal affected zone (TAZ). This energy is equivalent to the heat quantity that must be injected in the heat propagation equation. In the case of a semi-infinite medium with fusion temperature at the surface, the resolution of the heat propagation equation gives access to the width of the TAZ.     

铸态AZ31镁合金强流脉冲离子束改性

利用强流脉冲离子束（C+,H+）对变形镁合金AZ31的压铸件靶材分别进行1,5,10,20,30,50和100次辐照实验,分析辐照前后表面形貌和相组成,并检测辐照表面及横截面沿深度方向显微硬度。结果表明:HIPIB辐照次数对靶材形貌影响较大,多次辐照使靶材熔坑呈周期性变化趋势;-Mg17Al12相弥散分布于-Mg相中。1～30次辐照,表面显微硬度提高,其主要原因为晶粒细化及微应变导致的晶体缺陷;30～50次辐照,显微硬度显著降低,其原因在于晶体缺陷的演变,如位错移动导致的小角度晶界形成,甚至出现回复再结晶过程;50～100次辐照表面显微硬度略有降低,其原因在于辐照表面组织结构及热力学行为达到稳定态。辐照效应形成冲击应力波导致长程硬化,20次辐照的横截面显微硬度在距表层30 m和240 m处分别达到极大值1.0 GPa和1.3 GPa。     

Numerical and experimental study of the Ti6Al4V macrostructure obtained by Nd:YAG laser

Titanium and its alloys (Ti6Al4V) have been widely used in the biomedical field; nevertheless, they should be subject to specific surface treatments, before being implanted, in order to improve bio-integration. Although laser processing is a useful technique for this purpose, different aspects of the basic mechanisms of this process are still in progress, with special emphasis on the modeling structure formation on the irradiated surface. For this research, the finite element method was used to study the generation of a macrostructure on the Ti6Al4V surface using a Nd:YAG laser. The temperature profiles, estimated during the extremely high heating and cooling rates caused by the output power of the laser beam, allowed us to analyze, among other things, the melting depth and the heat affected zone, in order to optimize the process. Moreover, the experimental results (SEM data) were positively compared with the numerical model, and a relationship of the crater profile formation (depth to width ratio) was determined.     

表面状态对强流脉冲电子束辐照诱发金属表面熔坑的影响

 为了考察材料晶体学特性对表面熔坑形成机制的影响,利用强流脉冲电子束（HCPEB）对喷丸前、后的304奥氏体不锈钢进行表面辐照处理,对HCPEB诱发的表面熔坑形貌进行了详细的表征。实验结果表明,HCPEB辐照后样品表面形成了大量的火山状熔坑,熔坑数密度和熔坑尺寸随电子束能量的增加而减小,材料表面的杂质或夹杂物容易成为熔坑的核心,并在熔坑形成的喷发过程中被清除,起到净化表面的作用。此外,喷丸前、后样品表面熔坑数密度遵循相似的分布规律,喷丸处理使熔坑数密度显著增大,表明材料的晶体学特性对表面熔坑形成有重要的影响,晶界、位错等结构缺陷是熔坑形核的择优位置。