激光聚变实验装置屏蔽性能模拟计算北大核心CSCD

主要采用了蒙特卡罗方法对激光聚变实验装置外表面的中子和光子能谱及剂量进行模拟与分析,引入了MCAM软件绘制激光聚变实验装置的三维模型图,并自动转化为MCNP的输入文件,进行了靶室屏蔽性能的蒙卡模拟,从辐射防护的角度为屏蔽系统的建立、人员的辐射防护以及靶室材料的选择提供理论依据。通过模拟结果得出,CLAM钢作为靶室材料时,其屏蔽中子产生的瞬发光子剂量,在非孔道处是铝合金的1/2左右,40cm厚的混凝土屏蔽层对中子和光子起到了很好的屏蔽作用,均降低了一个数量级,另外在孔道处的中子和光子剂量,加了混凝土的情况反而比裸靶室时高10%左右,建议对靶室孔道外部考虑额外的防护。     

乏燃料贮运用铝基碳化硼复合材料的屏蔽性能计算

采用蒙特卡罗方法, 利用MCNP程序计算了在中子能量为0.5–20 MeV, ²³⁵U核热中子裂变源条件下, 厚度为3–9 cm、碳化硼含量5%–15%的铝基碳化硼复合材料在空气、水、200–1400 ppm (1 ppm=10^-6) 硼酸溶液介质中的中子透射系数. 结果表明: B₄C/Al复合材料的透射系数随碳化硼含量和材料厚度的增加而减少, 随中子能量的升高而增大, 而硼酸浓度的改变对中子透射系数影响不大. B₄C/Al复合材料在水中比硼酸中更能发挥其屏蔽效果, 在空气中屏蔽特性显现出“反转”现象, 中子能量高于5 MeV时透射系数几乎没有变化. 在裂变源条件下的B₄C/Al复合材料中子透射系数均比稳定源20 MeV 低. 介质的中子屏蔽效果是硼酸溶液>水> 空气, 水介质的中子透射系数与介质厚度呈指数下降关系, 裂变源和稳定源条件下分别近似为e^-0.71x和e^-0.669x, x为厚度(cm). 关键词： 蒙特卡罗 乏燃料设备 中子吸收材料 4C/Al')" href="#">B₄C/Al     

基于裂纹模板法的金属网格透明导电薄膜制备及性能改进

基于裂纹模板法制备了一种高屏蔽性能的金属网格透明导电薄膜.采用现有裂纹模板法制备得到的金属网格透明导电薄膜,其金属网格厚度较薄,屏蔽性能有待改进.本文在研究了裂纹材料的旋涂转速对龟裂图案的影响关系分布曲线中,增加了缝隙深度因子,选取了合适的裂纹材料和旋涂方案,制备得到理想的随机图案分布的裂纹模板.通过磁控溅射法在裂纹模板缝隙内外沉积厚度为1μm的金属层,引入了超声波清洗结合有机溶剂的方法,高效去除裂纹胶模板后,得到了金属网格透明导电薄膜样品.实测的金属网格透明导电薄膜样品透光率超过85%,同时方阻值保持在2.8Ω/左右,具有良好的透光和电磁屏蔽性能.通过制备加厚金属网格透明导电薄膜改进了屏蔽性能,为后续基于裂纹模板法制备高屏蔽性能金属网格透明导电薄膜提供了参考.     

基于Geant 4的介质深层充电电场计算

基于Geant4模拟了电子在Teflon介质中的电荷输运过程,获得了其内部的电流密度、剂量率和电荷沉积量沿深度的分布曲线,进而利用电荷连续性方程、泊松方程和深层俘获方程求解出Teflon中高能量、小束流电子辐照下的电场分布. 将介质平板充电过程简化为屏蔽铝板与分层介质组成的Geant4模型,电子源为1.0MeV,0.1pA/cm²的平面源. 通过记录经过各层介质的电子电量和各层介质内沉积能量和电子数目,用统计平均的方法获得了介质内电流密度、剂量率和电荷沉积量沿深度的分布规律. 介质内 关键词： 卫星 介质深层充电 Geant4 电场     

空间辐射环境及人体剂量蒙特卡罗模拟

针对空间辐射环境进行了理论分析,并使用蒙特卡罗方法,对银河宇宙射线及典型太阳质子事件进行了模拟。通过分析常规屏蔽对空间辐射场及人体剂量的影响、屏蔽下的次级粒子产额等,验证了蒙特卡罗工具包Geant4应用于空间辐射防护研究的准确性。模拟发现:在常规屏蔽厚度的情况下,对于太阳质子事件,由于其能量主要分布在低能量段(100 MeV以下),屏蔽效果随屏蔽厚度的增加明显增大,1 g/cm2 Al等效厚度屏蔽皮肤剂量可降低至其初始剂量值的8%左右,10 g/cm2 Al等效厚度的屏蔽可降低至初始剂量值的048%左右;而对于银河宇宙射线,由于其平均能量较高,屏蔽层的屏蔽作用并不明显,在浅层组织剂量甚至有所增加。     

SSRF前端区锯齿墙束流孔洞中子屏蔽的蒙特卡罗估算

主要关于上海同步辐射装置(SSRF)储存环电子引发产生的韧致辐射和中子辐射的研究.中子和光子经多种组合材料(厚度在5cm-115cm之间)屏蔽后的剂量特征由蒙特卡罗代码McNP和EGSnrc估算得到;蒙特卡罗计算表明,单一的材料如铅,铁和聚乙烯对高能中子是无效的生物屏蔽材料,而组合材料如铅或者铁加聚乙烯和铅或者铁加混凝土被认为是屏蔽高能中子很好的组合材料.铅铁等高Z材料加点包含有氢的低Z材料如聚乙烯是同时屏蔽高能中子和韧致辐射的一种比较好的组合材料选择.     

颗粒固体应力转向比的光弹法探测

利用压敏双折射光学特性材料,实验测量了在自然堆积和密堆积两种制样方式下颗粒仓轴向荷载在仓壁上随深度的分布.发现在填充颗粒总质量相同、容器不变的情况下,颗粒仓轴向荷载在仓壁上的分布不随颗粒深度单调变化,而是随深度呈单峰结构,数值模拟与实验观察定性符合,并且发现峰值依赖于荷载大小和样品的制备方式.另外,我们也测量了在不同填充高度下的颗粒底部平均应力随轴向荷载的变化,将其与边壁应力对比,得到颗粒体系不同深度处的转向比.     

SSRF前端区锯齿墙束流孔洞中子屏蔽的蒙特卡罗估算

主要关于上海同步辐射装置(SSRF)储存环电子引发产生的韧致辐射和中子辐射的研究. 中子和光子经多种组合材 料(厚度在5cm～115cm之间)屏蔽后的剂量特征由蒙特卡罗代码MCNP和EGSnrc估算得到; 蒙特卡罗计算表明, 单一的材料如铅, 铁和聚乙烯对高能中子是无效的生物屏蔽材料, 而组合材料如铅或者铁加聚乙烯和铅或者铁加混凝土被认为是屏蔽高能中子很好的组合材料. 铅铁等高Z材料加点包含有氢的低Z材料如聚乙烯是同时屏蔽高能中子和韧致辐射的一种比较好的组合材料选择.     

基于线变换的椭圆柱外隐身斗篷的设计研究

基于线变换方法与互补媒质理论提出了线变换下的椭圆柱外隐身斗篷,并得到了相应外隐身斗篷材料本构参数张量的表达式.根据导出的本构参数张量,利用电磁仿真软件分别对不同长度线段的外斗篷进行了仿真验证,仿真结果证实了所得到的本构参数张量的正确性.这种外斗篷的材料参数只在轴向变化,横向参数为常数,易于用超介质制备.考虑到损耗对隐身效果的影响,得到了引入损耗后的外斗篷磁场分布.最后给出了本构参数的分布.本文的研究为利用超介质制备外隐身斗篷提供了一种新的可行的方法.     

注氦尖晶石的红外光谱研究

利用傅立叶变换红外光谱仪对注He尖晶石样品随退火温变化而引起光吸收性能的变化进行了研究。发现尖晶石样品在626.4cm^-1附近的吸收峰随注入剂量的增加向小波数方向移动,而在随后退火过程该吸收峰随退火温度的增加而向大波数方向回复。该吸收峰的回复行为依赖于注入剂量和退火温度。认为在626.4cm^-1附近吸收峰随注入剂量和退火温度的这种变化与尖晶石中He的俘获以及释放有关。     

Pulse laser ablation at water–air interface

We studied a new pulse laser ablation phenomenon on a liquid surface layer, which is caused by the difference between the refractive indices of the two materials involved. The present study was motivated by our previous study, which showed that laser ablation can occur at the interface between a transparent material and a gas or liquid medium when the laser pulse is focused through the transparent material. In this case, the ablation threshold fluence is reduced remarkably. In the present study, experiments were conducted in water and air in order to confirm this phenomenon for a combination of two fluid media with different refractive indices. This phenomenon was observed in detail by pulse laser shadowgraphy. A high-resolution film was used to record the phenomenon with a Nd:YAG pulse laser with 10-ns duration as a light source. The laser ablation phenomenon on the liquid surface layer caused by a focused Nd:YAG laser pulse with 1064-nm wavelength was found to be followed by the splashing of the liquid surface, inducing a liquid jet with many ligaments. The liquid jet extension velocity was around 1000 m/s in a typical case. The liquid jet decelerated drastically due to rapid atomization at the tips of the ligaments. The liquid jet phenomenon was found to depend on the pulse laser parameters such as the laser fluence on the liquid surface, laser energy, and laser beam pattern. The threshold laser fluence for the generation of a liquid jet was 20 J/cm². By increasing the incident laser energy with a fixed laser fluence, the laser focused area increased, which eventually led to an increase in the size of the plasma column. The larger the laser energy, the larger the jet size and the longer the temporal behavior. The laser beam pattern was found to have significant effects on the liquid jet’s velocity, shape, and history.     

Surface modification of the titanium implant using TEA CO2 laser pulses in controllable gas atmospheres - Comparative study

Interaction of a TEA CO₂ laser, operating at 10.6 μm wavelength and pulse duration of 100 ns (FWHM), with a titanium implant in various gas atmospheres was studied. The Ti implant surface modification was typically studied at the moderate laser beam energy density/fluence of 28 J/cm² in the surrounding of air, N₂, O₂ or He. The energy absorbed from the TEA CO₂ laser beam is partially converted to thermal energy, which generates a series of effects, such as melting, vaporization of the molten material, shock waves, etc. The following titanium implant surface changes and phenomena were observed, depending on the gas used: (i) creation of cone-like surface structures in the atmospheres of air, N₂ and O₂, and dominant micro-holes/pores in He ambient; (ii) hydrodynamic features, most prominent in air; (iii) formation of titanium nitride and titanium oxide layers, and (iv) occurrence of plasma in front of the implant. It can be concluded from this study that the reported laser fluence and gas ambiences can effectively be applied for enhancing the titanium implant roughness and creation of titanium oxides and nitrides on the strictly localized surface area. The appearance of plasma in front of the implants indicates relatively high temperatures created above the surface. This offers a sterilizing effect, facilitating contaminant-free conditions.     

13.5—14·6 MeV能区中子引起的89Y39（n，2n）88Y39反应截面的测量

用^93Nb（n,2n）^92mNb和^90Zr（n,2n）^89m＋gZr截面比法测定中子能量,以^93Nb（n,2n）^92mNb反应截面作中子注量标准,用活化法测量了13．5-14．6MeV中子引起的^89Y（n,2n）^88Y的反应截面值。由（13．5±0．3）,（14.1±0．2）,（14.6±0．3）MeV中子引起的^89Y（n,2n）^88Y反应截面值分别为（759±42）,（835±42）和（958±53）mb。Cross section for （n, 2n） reaction on Yttrium have been measured at energy of 14 MeV neutrons from H（d, n）He by using activation technique. The ^93Nb（n, 2n）^92mNb reaction was used to monitor the neutron fluence, HPGe detector was used to detect the γ-rays. The cross section of ^89Y （n, 2n）^88Y reaction are 759 ± 42, 835 ±42, 958 ±53 mb for neutron energy 13.5 ±0.3, 14.1±0.2, 14.6 ±0.3 MeV, respectively.     

Development of a new nanocrystalline alloy for X-ray shielding

The purpose of this study was to develop a new nanocrystalline alloy material, which can replace lead for the purposes of radiation shielding as it is not hazardous to the human body and it is light in weight, to use the developed alloy in a fiber, and to evaluate its performance. This study used tungsten carbide and cobalt as the base metals and developed a new nanocrystalline alloy material. Then, radiation-shielding fibers 0.2 and 0.4?mm thick were created from the prepared tungsten carbide and cobalt powder. Equivalent dose was measured and shielding rate was obtained by the lead-equivalent test method for X-ray protection of goods suggested in the Korean Standard. According to our results, the shielding rate of the 0.2-mm-thick WC–Co alloy was 96.52% at a tube voltage of 50?kVp, 94.86% at a tube voltage of 80?kVp, and 94.10% at a tube voltage of 100?kVp. The shielding rate of the 0.4-mm-thick WC–Co alloy was 97.47% at a tube voltage of 50?kVp, 96.57% at a tube voltage of 80?kVp, and 95.63% at a tube voltage of 100?kVp. It is believed that the nanocrystalline WC–Co alloy developed for radiation shielding in this study will contribute to a decrease in primary X-ray exposure as well as exposure to low-dose secondary X-rays, such as scattered rays. Furthermore, the use of a nanocrystalline WC–Co alloy oxide rather than lead will allow for the development of shielding wear that is lighter and contribute to the development of various radiation-shielding products made of environmentally friendly materials.     

氮原子、分子与团簇离子注入Si(111)的特性研究

用椭偏仪、傅氏变换红外吸收谱(FTIR)、X射线光电子能谱(XPS)以及原子力显微镜(AFM)对N⁺₁,N⁺₂,N⁺₁₀离子高剂量(1.7×10¹⁷ions/cm²)注入Si(111)的表面进行测试分析,发现三种不同尺度的离子注入后,均使Si由复折射率变化为实折射率,表面出现含氮硅键的介质层.但其表面形貌各异:N^{+关键词： 氮团簇注入 表面特性}     

ASPIRE: An automated sample positioning and irradiation system for radiation biology experiments at Inter University Accelerator Centre,New Delhi

An automated irradiation setup for biology samples has been built at Inter University Accelerator Centre (IUAC), New Delhi, India. It can automatically load and unload 20 biology samples in a run of experiment. It takes about 20 min [2% of the cell doubling time] to irradiate all the 20 samples. Cell doubling time is the time taken by the cells (kept in the medium) to grow double in numbers. The cells in the samples keep growing during entire of the experiment. The fluence irradiated to the samples is measured with two silicon surface barrier detectors. Tests show that the uniformity of fluence and dose of heavy ions reaches to 2% at the sample area in diameter of 40 mm. The accuracy of mean fluence at the center of the target area is within 1%. The irradiation setup can be used to the studies of radiation therapy, radiation dosimetry and molecular biology at the heavy ion accelerator.     

Modification of engineering silicon nitride ceramics by energetic-ion bombardment

The microstructural and mechanical properties of hot-pressed Si₃N₄ ceramics after Si⁺ ion bombardent and annealing in N₂ atmosphere have been investigated as a function of the ion fluence and the annealing temperature. The irradiations were carried out at target temperatures of about 80 K and 450 K with ion energies of 0.5 MeV and 1.0 MeV. In all cases the fluence range was subdivided into two regimes: a low-fluence regime with improved microhardness and fracture toughness, and a high-fluence regime with an absolute degradation of these properties. The transition fluence was found to strongly depend on the ion energy and implantation temperature. This property transition coincides with a microstructural transition from a highly damaged, but still crystalline material, to the formation of a buried amorphous layer. The amorphization results in a strong volume swelling which causes a closure of surface flaws. The latter process significantly enhances the fracture strength of the implanted material. Thermal relaxation of the modified mechanical properties was found to occur at temperatures above 800° C. The relationships between the ion-induced changes of the mechanical properties and the microstructural modifications will be discussed.     

Ti离子注入和退火对ZnS薄膜结构和光学性质的影响

利用真空蒸发法在石英玻璃衬底上制备了ZnS薄膜,将能量80 keV,剂量1×10¹⁷ cm^-2的Ti离子注入到薄膜中,并将注入后的ZnS薄膜进行退火处理,退火温度500—700 ℃.利用X射线衍射（XRD）研究了薄膜结构的变化,利用光致发光（PL）和光吸收研究了薄膜光学性质的变化.XRD结果显示,衍射峰在500 ℃退火1 h后有一定程度的恢复;光吸收结果显示,离子注入后光吸收增强,随着退火温度的上升,光吸收逐渐降低,吸收边随着退火温度的提高发生蓝移;PL显示,薄 关键词： ZnS薄膜 离子注入 X射线衍射 光致发光     

超短脉冲激光在DBASVP分子中传播时的双光子面积演化和光限幅效应

以一维不对称π共轭分子体系（DBASVP分子）为介质,在双光子共振条件下,从双光子面积定理和严格数值求解Maxwell-Bloch方程两方面出发,分别研究超短脉冲激光在该有机分子介质中的传播过程,从而探讨双光子面积的演化规律,并分析双光子面积定理的适用性.提出了一种数值模拟分子介质光限幅特性的理论方法.分子的电子结构和电偶极矩是基于密度泛函理论利用从头计算方法得到的.研究结果表明,基于慢变幅和慢变相近似以及单模场条件下的双光子面积定理不能很好地描述超短脉冲的双光子面积在该分子介质中的演化规律.基于双光子吸收的分子光限幅特性与分子介质的厚度有关. 关键词： 双光子吸收 光限幅效应 双光子面积定理 超短脉冲激光     

Surface free energy of ultra-high molecular weight polyethylene modified by electron and gamma irradiation

Surface free energy of biocompatible polymers is important factor which affects the surface properties such as wetting, adhesion and biocompatibility. In the present work, the change in the surface free energy of ultra-high molecular weight polyethylene (UHMWPE) samples, which is produced by electron beam and gamma ray irradiation were, investigated. Mechanism of the changes in surface free energy induced by irradiations of doses ranging from 25 to 500 kGy was studied. FTIR technique was applied for sample analysis. Contact angle measurements showed that wettability and surface free energy of samples have increased with increasing the irradiation dose, where the values of droplet contact angle of the samples decrease gradually with increasing the radiation dose. The increase in the wettability and surface free energy of the irradiated samples are attributed to formation of hydrophilic groups on the polymer surface by the oxidation, which apparently occurs by exposure of irradiated samples to the air.