质子辐照不锈钢中氢气泡产生和演化研究

采用质子辐照模拟方法和正电子湮没寿命测量方法研究了质子辐照在国产改进型316L不锈钢中产生的氢气泡及其随辐照质子注量的演化过程。5×10^12,5×10^13,5×10^14／cm^2质子辐照的实验结果表明,辐照在不锈钢中产生氢气泡的尺度随辐照质子注量增加而增大,在质子注量为5×10^14／cm^2时氢气泡尺寸达到0．62nm,气泡的浓度随质子注量增加而减小。The bubble production and evolution in the home-made modified 316L stainless steel have been investigated by the proton irradiation simulation technique and the positron annihilation lifetime measurement. The experimental results of 5 × 10^12, 5 × 10^13 and 5 × 10^14/cm^2 proton irradiations show that the produced bubble size increases, while the bubble concentration decreases, with the increasing of the irradiation proton flueence. At the proton irradiation fluence of 5 × 10^14/cm^2 the bubble size reaches 0.62 nm.     

Study of magnetic-rotation in ~(82)Rb by g-factor measurements

Magnetic rotation in ⁸²Rb has been investigated for the first time by g-factor measurement of intra-band states of the magnetic-rotational band built on the 11- state. The g-factors were measured by a TMF-IMPAD method and calculated by a semi-classical model of independent particle angular momentum coupling assumption. The g-factors and deduced shears angles decrease with the increasing of spin along the band, illustrating a step-by-step alignment of the valence protons and neutrons. The rapid alignment of the valence neutrons leads to a decrease of g-factors. The present results vividly reveal the shears mechanism of magnetic rotation.     

蛋白A高效亲和膜色谱法测定人血浆中免疫球蛋白G的含量

研究了蛋白Ａ高效亲和膜色谱对水溶液及人血浆中人免疫球蛋白Ｇ（ＨＩｇＧ）的特异性吸附和定量测定。方法具有较高的精确度和较好的重复性：ＨＩｇＧ标样５次重复进样的相对标准偏差为１．５％，人血浆样品３次重复进样的相对标准偏差为３．６％；所测得的定量标定曲线的线性相关系数达到０．９９９３；不含己二胺间隔臂的亲和介质的非特异性吸附极低，基本检测不出来。快速实验中，一次分析可在０．５ｍｉｎ内完成。实验表明，利用所建立的方法对人血浆中的ＨＩｇＧ进行定量测定可以得到较为满意的结果。     

Magnetic moment measurements of mirror nuclei 12B and 12N

The spin polarized β-emitting mirror nuclei ¹²B(I^π=1⁺,T_1/2=20.18 ms) and ¹²N(I^π=1⁺,T_1/2=11 ms) are produced by the low nuclear reactions ¹¹B(d, p) ¹²B and ¹⁰B(³He,n) ¹²N and by selecting the projectile energy and the recoil angle. Their magnetic moments are measured by the β-NMR technique. The magnetic moments obtained after Knight shift correction are μ(¹²B)=1.001(17) μ_N and μ(¹²N)=0.4571(1) μ_N. The calculation using the existing shell model could not reproduce the measured magnetic moments for ¹²B and ¹²N simultaneously.     

复合纤维素金属螯合膜色谱介质的制备及其分离生物大分子的研究

以棉纤维为基质 ,通过聚合、接枝、开环反应合成了亚氨二乙酸型金属螯合复合膜色谱介质 ,考察了反应温度 ,反应时间对合成介质性能的影响 ,并对复合纤维素膜的表面物理性能及蛋白质的结合性能进行了表征 .实验结果表明 ,膜色谱介质对蛋白质具有较大的吸附容量 ,分离效果与凝胶介质相当 ,但分离速度快 3～ 5倍 .复合膜色谱介质还具有负压低 ,成本低 ,使用寿命长等特点 ,适于生物大分子的快速大规模分离纯化 ,并用于高效液相色谱对生物大分子的快速定量分析 .     

不锈钢辐射损伤随温度和剂量的变化(英文)

用重离子辐照模拟和正电子湮没寿命技术研究了改进型316L不锈钢在21 和33 dpa辐照剂量下的辐照损伤在室温到802 °C温度范围随辐照温度变化和室温下0—100 dpa剂量范围随辐照剂量变化. 在580 °C左右实验观察到辐照肿胀峰， 在21 和33 dpa辐照剂量下相应的空位团分别由14和19个空位组成， 尺度分别为0.68 和0.82 nm. 空位团尺寸随辐照剂量增加， 在100 dpa时空位团由8个空位组成， 尺度为0.55 nm. 实验结果表明， 在改进型316L不锈钢中辐照损伤随辐照温度变化更灵敏.     

火焰原子吸收光谱法测定铼产品中的痕量钠

建立了火焰原子吸收光谱法测定高铼酸、高铼酸铵、铼粉中痕量钠的方法,对样品的预处理和测定钠的条件进行了研究。结果表明:水溶解法、硝酸溶解法或硝酸-硫酸溶解法溶解样品完全,测得钠的结果吻合;于选定条件下,钠的测定浓度在0.020 0~0.500 0μg/mL范围内线性良好;测定高铼酸、高铼酸铵和铼粉样品中0.27~0.47mg/L、0.000047%~0.00048%和0.000040%~0.00049%的钠含量,检出限、相对标准偏差(RSD,n=7)、加标回收率分别为高铼酸3×10-4μg/mL、6%~10%、98%~102%,高铼酸铵3×10-4μg/mL、8%~9%、96%~102%和铼粉3×10-4μg/mL、5%~9%、96%~103%。方法结果准确、分析快速、操作简便,应用于实际的样品分析,结果满意。     

Structure of β-emitting nuclei 29P

The extoic structure of ²⁹P was investigated by measuring its magnetic moment in the ground state with β-NMR method. We got the experimental value of 1.2346 μ_N after diamagnetism correction. It is very close to the calculated value of 1.1009 μ_N computed with shell model. The shell model calculation also gave a proton density distribution of ²⁹P with a long tail. The present results show that 2s_1/2 proton in the ²⁹P may lead to the proton-skin structure.     

Proton alignment in 82Sr investigated by g-factor measurements

The proton alignment in ⁸²Sr has been investigated by the g-factor measurements of the ground state rotational band levels up to spin I=8⁺. The g-factors were measured by a transient-magnetic-field ion implantation perturbed angular distribution method. The obtained g-factors increase with the increasing of spin along the band and clearly show the g_9/2 proton alignment that starts at I=6⁺.