^176Hf（n,2n）^175Hf和^185Re（n,2n）^184Re^m,g反应截面研究

用中国原子能科学研究院ＨＩ－１３串列加速器,高压倍加器和北京大学４．５ＭＶ静电加速器分别获得能量为１０－１２,１４和１８ＭｅＶ的中子,了＾１７６Ｈｆ（ｎ,２ｎ）和＾１８５Ｒｅ（ｎ,２ｎ）的反应堆面,并与现有的实验数据作了比较,初步搞清了分歧的主要原因和激发函数的走向。     

~(107)Ag(d,2n)~(107)Cd和~(109)Ag(d,2n)~(109)Cd反应的激发函数

用13.4MeV的氘束轰击天然银迭靶,银箔前后用铝箔作捕集减能膜。实验确定了~(107)Ag(d,2n)~(107)Cd和~(109)Ag(d,2n)~(109)Cd反应的激发函数,同时作了理论计算。由结果可见,实验值与理论值吻合得很好。     

非晶态合金（Fe1—xYx）84B16的穆斯堡尔谱学和磁学研究

用穆斯堡尔效应和磁测量方法对非晶态薄带(Fe_(1-x)Y_x)_(84)B_(16)(0≤x≤0.21)进行了研究。实验结果证实在所研究的样品中存在短程有序相互作用和由于钇替代而产生的不均匀区域。     

In_(0.95)Ag_(0.045)Ga_(0.005)合金中的电四极相互作用

本文采用时间微分扰动角关联方法,测量了80—422K温度范围内~(111)Cd在In_(0.95)Ag_(0.043)Ga_(0.005)合金中的四极相互作用随温度的变化,进而导出晶格电场梯度的温度变化。在In_(0.95)Ag_(0.043)Ga_(0.005)合金中,晶格电场梯度的温度变化遵从T~(3/2)定律:V_(zz)(T)=V_(zz)(0)(1—BT~(3/2)),斜率B=7.48(47)·10~(-5)K~(-3/2)。在80、298和422K的电场梯度分布宽分别为0.1147(259)、0.0924(340)和1.344(175)。表明在液氮温度和室温时,合金的晶格结构特性较好,温度升高,晶格结构特性变坏。     

~(89)Y(n,2n)~(88)Y反应截面测量

利用活化法的基本原理和相对测量方法,测量得到13.5～14.8MeV的D-T中子作用下的89Y(n,2n)88Y反应截面。89Y(n,2n)88Y反应截面为629～1053mb,相对不确定度为1.7%。并与采用大液闪测量的实验结果和ENDF/B-6库的截面数据进行了比较,当中子能量为14.1MeV处ENDF/B-6数据与实验值的比值为0.99。     

间位碘代苄胍硫酸盐的合成和快速标记

本文介绍了用碘代芳烷基溴与游离胍缩合,合成了肾上腺髓质显像剂——间位碘代苄胍硫酸盐(MIBG sulfate);同时介绍了放射性碘标记MIBG的快速标记方法——热液熔融法;探讨了标记的最佳条件,确定标记反应温度为170—180℃、反应时间为1h、溶液体积为20—25μl,标记率可达95％。     

Isospin Distribution of Fragments in Reaction ~(96)Ru ~(96)Ru, ~(96)Ru ~(96)Zr,~(96)Zr ~(96)Ru,and ~(96)Zr ~(96)Zr at Beam Energy 400 AMeV

The isospin distribution of particles and fragments in collisions 96Ru 96Ru, 96Ru 96Zr, 96Zr 96Ru, and 96Zr 96Zr at beam energy 400 AMeV is studied with isospin dependent QMD model. We find the rapidity distribution of difference between neutron-proton number in neutron rich nucleus-nucleus collisions at intermediate energies is sensitive to the isospin dependent part of nuclear potential. The study of the N/Z ratio of nucleons, light charged particles (LCP) and intermediate mass fragments (IMF) shows that the isospin dependent part of nuclear potential drives IMF to be more isospin symmetric and emitted nucleons to be more neutron rich. We also study the time evolution of the isospin distribution     

Kinetic study on Iigand-exchange reaction between ethylenedicysteine (EC) and ~(99m)Tc-glucoheptonate (~(99m)Tc-GH)

A detailed kinetic study of ligand-exchange reaction between 99mTc-GH and EC was carried out. The rate constants (k) of ligand-exchange reaction at different EC concentrations and different pH values were calculated. The k values (L · mol-1 · min-1) were 3.7 × 103, 4.1 × 103, 3.9 × 103 and 3.9 ×88 103 at EC concentrations (μmol · L-1) of 559.7, 279.9, 186.6 and 55.97, respectively, while k values were 3.7×103, 3.4×103, 1.9×103 and 3.1×88 102 when pH values were 10, 9, 8 and 7, respectively, and k had an increase of the order of magnitude from pH 7 to pH 8. It demonstrated that k of the ligand exchange reaction was pH dependent and pH value of the reaction solution must be equal to or little higher than 8 in order to make the labeling yield of 99mTc-EC higher than 90%.     

掺Pb超导体（Bi2—xPbx）Ca2.5Nd0.5Cu2O8＋y的正电子寿命研究

室温测量了（Ｂｉ２－ｘＰｂｘ）Ｃａ２．５Ｎｄ０．５Ｃｕ２Ｏ８＋ｙ超导体的正电子寿命与Ｐｂ含量的关系。在２２１２相发现随着Ｐｄ含量的增加正电子体寿命相应地减小，分析表明，这是由于Ｐｂ替换了Ｂｉ，使电子从Ｃｕ－Ｏ面或其它晶位迁移到Ｂｉ－Ｏ层，并导致Ｂｉ－Ｏ层电子密度增加所致。     

^179Hf（n,2n）^178Hf^m2和^209Bi（n,2n）^208Bi反应截面的测量

用活化法测量相对于~(93)Nb(n,2n)~(92)Nb~m反应的~(179)Hf(n,2n)~(178)Hf~(m2)的反应截面和相对于~(27)Al(n,2n)~(24)Na反应的~(209)Bi(n,2n)~(208)Bi的反应截面。在中子能量为14.4 MeV处~(179)Hf(n,2n)~(178)Hf~(m2)反应的测量截面为(6.04±0.32)×10~(-31)m~2。在中子能量为14.6 MeV处~(209)Bi(n,2n)~(208)Bi反应的测量截面为(2279±173)×10~(31)m~2。在这些测量中,中子能量是用~(90)Zr(n,2n)~(89)Zr~(m+8)反应和~(93)Nb(n,2n)~(92)Nb~m反应的截面比法测定的。