利用同质异位素产额比提取对称能的近似方法

在修改的Fisher模型框架下, 利用同质异位素产额比和结合能方程中对称能系数与温度比率的关联, 可以提取对称能系数与温度的比值。 利用3种不同的近似方法得到了重离子核反应产生丰中子余核的对称能系数与温度比（a_sym/T）,并研究了相关物理量对a_sym/T的影响。结果表明, 库仑能对提取丰中子余核的a_sym/T影响较小,且参考核的选取对a_sym/T的提取也有一定的影响。 In the framework of the modified Fisher model, correlations between the symmetry energy coefficient in semi classical mass formula to temperature (a_sym/T) and the isobaric yield ratio in Heavy ion collisions are established. a_sym/Tof neutron rich fragments are extracted using these correlations. It is found that the Coulomb energy term has little effect on a_sym/T of fragments, while the reference isobars adopted have great influence on the extracted a sym/T of fragments.     

原子模型理论的参数确定与检验方法

根据多电子原子价电子径向波函数的节点特性，结合光谱实验数据，提出了一种确定与检验原子模型势理论中势参数的方法，使所得的波函数避免了因内层电子波函数的混入而造成的坍陷。     

2D/3D ZnIn2S4/TiO2复合物的原位构筑及其提高的光催化性能

通过高温煅烧和油浴的方法构筑二维/三维(2D/3D) ZnIn₂S₄/TiO₂异质结, 应用于光催化降解罗丹明B (RhB)和四环素(TC), 来研究异质结的构筑对TiO₂可见光响应范围和光生载流子对分离效率的影响. 结果表明, TiO₂维持了MOFs的形貌, 显示窄的可见光响应范围和高的光生电荷复合率, 与ZnIn₂S₄纳米片复合后, TiO₂的比表面积增大, 光催化活性位点增多. 带隙宽度也由TiO₂的3.23 eV减小到ZnIn₂S₄/TiO₂-II的2.52 eV, 从而获得了更宽的可见光响应范围. 能带结构表明ZnIn₂S₄/TiO₂是type II型异质结, 提高了光生载流子对的分离与转移效率. 在可见光照射下, ZnIn₂S₄/TiO₂-II显示了最高的RhB光催化降解效率(93%), 分别是TiO₂和ZnIn₂S₄的18和2倍. 同时, ZnIn₂S₄/TiO₂-II也显示出比TiO₂和ZnIn₂S₄更高的TC降解效率(90%). 循环实验表明ZnIn₂S₄/TiO₂-II能保持良好的稳定性, 经5次循环实验后仍能降解83%的RhB. 研究表明基于MOFs衍生的TiO₂构筑2D/3D ZnIn₂S₄/TiO₂异质结是提高TiO₂光催化性能的一条有效途径.     

原子模型势理论中径向微分算符矩阵元的计算

本文推广［７，８］的工作，导出了多电子原子模型势理论中含径向微分算符的矩阵元通式，可直接用于以“速度”及“加速度”形式跃迁振子强度计算。     

New experimental measurement of natSe(n, γ) cross section between 1 eV to 1 keV at the CSNS Back-n facility

The ⁷⁴Se is one of 35 p-nuclei, and ⁸²Se is a r-process only nucleus, and their (n, γ) cross sections are vital input parameters for nuclear astrophysics reaction network calculations. The neutron capture cross section in the resonance range of isotopes and even natural selenium samples has not been measured. Prompt γ-rays originating from neutron-induced capture events were detected by four C₆D₆ liquid scintillator detectors at the Back-n facility of China Spallation Neutron Source (CSNS). The pulse height weighting technique (PHWT) was used to analyze the data in the 1 eV to 100 keV region. The deduced neutron capture cross section was compared with ENDF/B-VIII.0, JEFF-3.2, and JENDL-4.0, and some differences were found. Resonance parameters were extracted by the R-matrix code SAMMY in the 1 eV-1 keV region. All the cross sections of ^natSe and resonance parameters are given in the datasets. The datasets are openly available at http://www.doi.org/10.11922/sciencedb.j00113.00019.     

A revisit to the neutron skin thickness of neutron-rich nuclei in the statistical abrasion ablation model

The cross sections of the fragments produced in the projectile fragmentation reactions of the even calcium isotopes from A=36 to A=52 are calculated using the statistical abrasion ablation model.The neutron skin thickness are studied by investigating the fragments isotopic cross section distributions.The neutron-skin thicknesses of the calcium isotopes have a good linear correlation to the peak positions of their fragment isotopic cross section distributions.The correlation between the neutron skin thickness and the neutron density distributions of 48 Ca is investigated by introducing a parameter to adjust the diffuseness parameter in the fermi-type density distribution.     

CrTiAlN涂层在800℃和900℃时对H13钢氧化性能的影响

为了提高H13钢的抗高温氧化能力,在H13钢表面沉积了一层CrTiAlN薄膜.采用XRD和SEM分析了H13钢氧化前后的相组成及其表、截面形貌.结果表明:涂层为柱状晶结构,主要有三部分组成:里层为Cr结合层,中间为CrN过渡层,外层是CrTiAlN梯度涂层.H13钢在氧化时,在其表面发生了Cr的选择性氧化,但是Cr含量低,未能形成连续的防护层,最终导致基体元素不断地氧化,生成了大量的α-Fe2O3颗粒.CrTiAlN涂层在800℃时具有良好的抗高温氧化性能,涂层氧化时主要是O向里扩散占优势,没有出现裂纹和剥落,而且观察到了“钉扎效应”.900℃时,涂层失效.     

Pairing-energy coefficients of neutron-rich fragments in spallation reactions

The ratio of pairing-energy coefficient to temperature(a_p/T)of neutron-rich fragments produced in spallation reactions has been investigated by adopting an isobaric yield ratio method deduced in the framework of a modified Fisher model.A series of spallation reactions,0.5A and 1A Ge V~(208)Pb+p,1A Ge V~(238)U+p,0.5A Ge V~(136)Xe+d,0.2A,0.5A and 1A Ge V~(136)Xe+p,and~(56)Fe+p with incident energy ranging from 0.3A to 1.5A Ge V,has been analysed.An obvious odd-even staggering is shown in the fragments with small neutron excess(I≡N-Z),and in the relatively small-A fragments which have large I.The values of a_p/T for the fragments,with I from 0 to36,have been found to be in a range from-4 to 4,and most values of a_p/T fall in the range from-1 to 1.It is suggested that a small pairing-energy coefficient should be considered in predicting the cross sections of fragments in spallation reactions.It is also concluded that the method proposed in this article is not good for fragments with A/A_s85%(where A_(s )is the mass number of the spallation system).     

外加磁场微波等离子推力器内流场数值模拟

为了提高微波等离子推力器性能，改善等离子体对电磁波能量的吸收状况，提高核心区温度，提出外加磁场的方案，并对热等离子体进行了数值模拟.假设局域热平衡条件，采用Navier-Stokes，Maxwell和Saha方程，利用压力修正的半隐格式和时域有限差分求解方法，建立了径向磁镜场下推力器内等离子体流场的数值计算模型.数值模拟结果表明：外加磁场后的磁感应强度小于0.5 T时，推力器内热等离子体核心区最高温度随磁感应强度的增加而迅速提高.外加磁场后的磁感应强度大于0.5 T时，核心区最高温度随磁感应强度的增加而缓慢提高.磁感应强度为0.5 T时，热等离子体核心区最高温度与不加磁场相比提高了24%.外加磁场对等离子体流场速度分布影响不大. 关键词： 等离子体模拟 等离子体相互作用 等离子体流动     

实验程序与教法探索

怎样才能组织好学生分组实验,特别是对于实验内容较多、技能训练要求较高的实验,按怎样的原则组织才能有效地激发学生的主动性和积极性,促使每一个学生认真投入到实验的每一个过程之中,以达到培养学生的实验技能和提高分析现象解决问题的能力呢?现按实验的一般程序谈谈我们的一些看法。学生分组实验的教学程序一般分准备、操作、总结三个阶段。