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1.
为满足对聚变堆面向等离子体材料中氘氚滞留问题的研究,北京大学4.5 MV静电加速器在原束线基础上新增核反应分析系统,该系统使用能量0.8~3.6 MeV的H~+、D~+、~3He~+和~4He~+粒子束流,可对核反应微分截面和样品中元素浓度的深度分布进行测量分析。本文对核反应分析原理、核反应分析系统的设备布局和实验方法进行了讨论,并以D(~3He,p)~4He核反应为例,分析了微分截面计算和样品中氘元素浓度深度分布的数据结果,其深度分辨小于1.5μm,实验误差约为7.5%。  相似文献   

2.
本文采用30 keV的He离子辐照Hastelloy N合金,辐照温度为500C,剂量分别为:1×1015、×1015、1×1016He+/cm2。利用扫描电子显微镜(SEM)研究了辐照后块体样品的表面形貌。结果表明,辐照后的块体样品均观察到了表面起泡现象。利用透射电子显微镜(TEM)研究了辐照后TEM样品微结构的变化。结果表明,低剂量(1×1015 He+/cm2)辐照的样品中出现了黑斑缺陷;随着辐照剂量的增加,开始出现位错环及纳米级的氦泡,同时黑斑密度减少;当剂量增至1×1016He+/cm2,位错环以及氦泡的尺寸和密度明显增大,晶界处氦泡更加密集。  相似文献   

3.
光核反应数据在辐射损伤、反应堆剂量、加速器屏蔽等方面有重要应用。本工作基于MEND-G程序,对200 MeV能量范围内光子诱发50,51V核反应数据进行理论计算,给出包含中子、质子、4He等主要出射粒子的核反应的数据;对光子诱发V同位素核反应的实验测量进行自洽性分析,结合光子强度函数和准氘模型,将光核反应吸收截面计算能力提升到200 MeV,为光核反应理论计算提供数据基础。经系统比对,理论计算值与实验测量值一致性很好,数据收录在即将发布的CENDL-3.2光核子数据库中。  相似文献   

4.
本文借助双核模型,进行了对多核子转移反应中前平衡结团发射机制进行了系统研究。以反应系统12C+209Bi、40Ca+208Pb和48Ca+238U为例,重点分析了库仑位垒附近重离子碰撞产生前平衡轻粒子,如中子、质子、氘核、氚核、3He、4He、6Li、7Li、8Be和9Be时间演化、动能分布和角分布。研究结果表明:结团发射呈现出一定核结构效应,4He发射概率与质子相当并远大于3He。前平衡结团主要分布在“类弹”和“类靶”角度区域发射,其动能分布呈现出玻尔兹曼分布形式。考虑结团预形成因子后该方法可以拓展用于不稳定原子核引起的结团发射机制研究。  相似文献   

5.
用热解吸和静态贮存方法对贮氚非晶态ZrV2合金膜中3He的释放行为进行了系统分析。结果显示:3He原子存在597.3、725.8和1 146.6 K等3个解吸峰,其中第3解吸峰的解吸量最大,是由非晶态基体中的3He释放形成;在长达2 423 d的静态贮存期间,非晶膜中3He原子的释放系数始终在10-5量级范围内波动并呈线性上升趋势,但仍未加速释放;贮存温度变化会引起释放系数剧烈波动;与贮氚晶态ZrV2合金膜相比,非晶膜的固氦能力显著增强。上述结果初步证实了非晶合金具有良好的固氦性能,这有助于人们从全新视角认识材料中的氦行为。  相似文献   

6.
本文对低能D(d,γ)4He聚变反应进行了实验研究。由于D(d,γ)4He聚变反应γ射线的产额低、能量高、本底大,实验采用大NaI-塑料闪烁体反康谱仪,以提高探测效率并降低宇宙线的影响;采用脉冲束飞行时间方法区分中子和γ射线,以减小中子和宇宙线本底的影响。实验测量了300 keV d束轰击厚D靶和薄D靶两种情况下的γ数据。在计算反应产生23.8 MeV的高能γ峰面积时,采用了拟合法扣除本底。实验测得,对厚靶,D(d,γ)4He反应截面为2.47×10-37m2;对薄靶,D(d,γ)4He反应截面为4.36×10-37m2。  相似文献   

7.
90Sr/90Y放射性衰变平衡体系中分离获得的90Y溶液具有无载体、金属杂质含量高等特点,需要进一步纯化才能应用于90Y放射性药物的制备。本工作研究了AE4强碱性阴离子交换树脂在盐酸溶液中对Y3+、Fe3+、Al3+、Zn2+、Mg2+的吸附性能。结果表明:AE4树脂在盐酸溶液中不吸附Al3+、Zn2+、Mg2+;在3 mol/L以上的盐酸溶液中对Fe3+吸附性能较好;在7 mol/L以上的盐酸溶液中对Y3+的吸附性能较好。含有Y3+、Al3+、Zn2+、Mg2+等元素的混合溶液在3 mol/L HCl溶液通过AE4树脂柱后,Fe3+基本被全部吸附在树脂柱上;吸附余液调节盐酸浓度至7 mol/L,通过另一根AE4树脂柱,Y3+基本被吸附在树脂柱上。最后用0.01 mol/L HCl洗脱吸附在树脂柱上的Y3+,得到纯化后的YCl3溶液。稳定核素和90Y示踪的研究结果表明,采用AE4树脂纯化90YCl3溶液的工艺可行,AE4树脂可用于90YCl3溶液中Fe、Al、Zn、Mg等主要杂质金属元素的去除。  相似文献   

8.
锂陶瓷氚增殖剂的氢同位素行为是聚变堆固态产氚包层关心的重要课题。本文将3 keV D+注入Li4SiO4,采用X射线光电子能谱在线分析注氘前后材料表面的化学状态,同时采用热解吸谱(TDS)实验技术,研究注氘后Li4SiO4中氢同位素的热解吸行为。实验结果表明:D+注入会改变Li4SiO4表面的化学环境,产生多种辐照缺陷和化学键合状态;氘滞留量和热解行为受注氘时样品的温度影响较大,可在一定程度上预测产氚包层中氚的滞留行为。  相似文献   

9.
中国原子能科学研究院核反应团队依托国内外的大科学装置,在重离子熔合-裂变机制、垒下熔合增强机制、奇特核反应机制、奇异结构和奇异衰变方面取得了多项原创性成果。本文对其中的代表性成果进行了简要回顾。主要包括(:1)系统调查了正Q值中子转移的耦合道效应,并提出了自洽的方法评估转移耦合的贡献,发现了异常的同位素效应;(2)提出了用高精度背角准弹散射方法抽取原子核的形变参数,确证了原子核存在十六极形变;(3)提出了用轻带电粒子的替代俘获反应方法,基于此方法给出了关键的239Pu(n,2n)反应截面;(4)系统考察了sd壳丰质子核奇异衰变谱学,发现了22Si的β缓发双质子衰变模式,并发现镜像核22Si/22O的β衰变中存在极大的同位旋不对称性,同时在26Si中发现了迄今为止最强的同位旋混合态(;5)系统研究了奇特核体系在近垒能区的反应机制,首次给出了实验证据表明经典色散关系不适用于中子晕核6He+209Bi体系,并对质子滴线核8  相似文献   

10.
武永伟  曾志  马豪 《辐射防护》2018,38(3):197-204
利用中国锦屏地下实验室(CJPL)低本底γ谱仪对北京地区近4年34组气溶胶样品中长寿命放射性核素进行研究。发现气溶胶样品中含有238U、226Ra、210Pb、232Th、228Ra、 40K、7Be、137Cs,其活度浓度均值分别为17.47 μBq·m-3、21.19 μBq·m-3、2.39 mBq·m-3、11.12 μBq·m-3、14.43 μBq·m-3、226.64 μBq·m-3、6.98 mBq·m-3、2.36 μBq·m-3,且均在本底范围之内。同时,放射性核素活度浓度与环境参数存在相关性,7Be、40K、137Cs、226Ra均与季节负相关,210Pb与季节正相关;40K与空气质量指数(AQI)正相关。  相似文献   

11.
The surface layer of beryllium-coated graphite was analysed by backscattering and nuclear reaction methods using a 2.5 MeV accelerator. For the Be analysis the nuclear reactions 9Be(p, d)8Be, 9Be(p, )6Li, 9Be(d, p)10Be, 9Be(d, t)8Be, 9Be(d, )7Li and 9Be(3He, p)11B are compared with backscattering of 4He+ and protons. For the analysis of carbon, which provides complementary information to the depth profiling of Be, and for the analysis of oxygen, which is the third element of importance in the system, elastic backscattering of 4He+ and protons is applied. It turns out that the backscattering analysis with protons of 1.3 MeV presents the best compromise for a quick and straightforward measurement of all three elements. The other methods have their merits for a more detailed analysis.  相似文献   

12.
An analytical procedure and a simulation-optimization algorithm are described for hydrogen determination based on elastic recoil detection induced by low-energy 4He ions ( 3 MeV) using transmission geometry. Hydrogen concentration depth profiles can be derived from the experimental recoil spectra for a depth range of up to 6 μm with a resolution better than 40 nm at the surface. The method is applied to thin polyimide films irradiated by high-energy heavy ions. The 3D hydrogen distribution is determined with a 4He+ mubeam. A high-hydrogen-concentration zone below the surface is shown. The hydrogen distribution is seen to evolve during the 4He+ irradiation.  相似文献   

13.
In order to get information about the lattice location and the mobility of 12C in GaAs wafers, the channeling technique in combination with nuclear reaction analysis (NRA) is a powerful method. The targets were implanted with 12C ions (2.6 × 1013−2.6 × 1015cm−2) at energies between 60 and 3000 keV. This corresponds to implantation depths of about 0.1 to 3 μm. Using the nuclear reaction 12C(d, p)13C a depth distribution of the implanted carbon is obtained. The relationship between the concentration of 14C in random and along the 100 and 110 axial directions gives information about the substitutional lattice location of carbon within the GaAs crystal. In addition, we measured lattice defect depth distributions with a 1.5 MeV 4He+ beam before and after thermal annealing at temperatures up to 600°C.  相似文献   

14.
Charged particle activation analysis (CPAA) is able to analyze light elements such as carbon and oxygen at trace levels in semiconductor materials. This technique requires the knowledge of the stopping powers of these materials for channeled ions. The electronic energy loss for ions entering the crystal lattice in a random direction is well established. The electronic energy losses for protons, deuterons, 3He+ and 4He+ ions entering a 3.6 μm thick silicon single crystal along the 1 0 0 direction were measured by using the transmission of particles technique. Data obtained were compared with those obtained by other authors using theoretical and experimental methods.  相似文献   

15.
为认识脉冲离子束作用下金属氚化物的氦释放行为,建立了脉冲离子束作用下金属氚化物氦释放测量系统。利用标准体积气体取样装置,采用气体反扩散法,对系统的容积比、灵敏度进行了实验标定。在此基础上,发展了脉冲离子束作用下金属氚化物氦释放的测量技术,开展了脉冲离子束作用下金属氚化物氦释放实验研究。结果显示,单次脉冲离子束作用下金属氚化物的氦释放呈脉冲式,释放量最大可达10~(13)个原子以上。  相似文献   

16.
由于受到放射性束强度弱、品质差的限制,奇特核体系的光学势性质一直是亟待解决的国际难题。本工作利用稳定束的转移反应作为探针,深入研究了反应出射道奇特核体系的光学势性质。利用中国原子能科学研究院的HI-13串列加速器在近库仑位垒能区高精度测量了7Li+63Cu、208Pb的弹性散射以及单质子转移反应角分布,并利用扭曲波玻恩近似(DWBA)和耦合反应道(CRC)方法对实验数据进行了拟合,抽取了出射道6He+64Zn、209Bi晕核体系的光学势参数。所得参数可重现文献中已有的6He体系的弹性散射角分布,验证了这种方法的可靠性。对所得势参数的能量相依性的分析表明,在重体系6He+209Bi中,基于因果律的色散关系并不适用,其潜在的物理原因还需进一步深入研究。  相似文献   

17.
18.
Activation techniques have been used to measure the cross section for the 41K(n,p)41Ar reaction between 14.2 and 17.2 MeV. Neutrons were produced by the 3H(d,n)4He reaction, and the mixed-power method was used to measure the neutron flux through the 27Al(n,)24Na reaction. The activated samples were counted for the 1294 keV, 1.827 h γ-activity of 41Ar and the 1369 keV, 15.03 h γ-activity of 24Na using a 16% Ge(Li) detector and a 4096-channel analyzer. The cross sections for the 41K(n,p)41Ar reaction using the mixed-power method were found to be 53 ± 3 mbarn at 14.2 ± 0.2 MeV, 47 ± 3 mbarn at 15.2 ± 0.2 MeV, 41 ± 3 mbarn at 16.2 ± 0.2 MeV and 36 ± 4 mbarn at 17.2 ± 0.2 MeV. The associated-particle method was also used for measuring the neutron flux in order to check the mixed-powder result at 14.2 MeV. The average cross section for three associated-particle runs at 14.2 MeV was found to be 50 ± 3 mbarn which, within experimental error, agrees with the mixed-powder value.  相似文献   

19.
The influence of the nuclear and electronic energy loss on the damage production in GaAs has been studied by Se+ ion implantation at TI = 293 K with energies ranging from 2 MeV up to 20 MeV. The ion dose was varied between 5 × 1012 /cm2 and 1 × 1015 /cm2. The damage production was investigated using RBS in channeling regime. Temperature and energy dependent backscattering measurements and TEM investigations were performed to study the kind of defects in more detail. The resulting defect profiles are compared with the depth distribution of the nuclear and electronic energy loss which were simulated by TRIM 87. The results show that the remaining defect concentration strongly decreases with increasing implantation energy even if the same energy density is deposited into nuclear processes. We suppose, that the electronic energy loss increases the defect transformation and annealing during implantation at TI = 293 K. The defects in the samples implanted with energies greater than 5 MeV are characterized as point defects, point defect clusters and small dislocation loops; the kind of defects are the same over the whole implantation depth and the existence of amorphous zones can be widely excluded.  相似文献   

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