12N直接碎裂反应研究

描述了在兰州放射性束流线(RIBLL)上用78.6MeV/u的¹⁴N束流轰击Be靶产生出34.9MeV/u的¹²N次级束流. 利用¹²N轰击Si靶作为次级靶, 利用直接碎裂反应测量它的反应总截面. 利用理论模型进行了计算, 理论计算和实验结果符合的很好. 发现¹²N的质子密度分布相对于中子而言, 有一个很大的弥散.     

透射法测量丰中子核8He的去中子截面

利用HIRFL提供的50MeV/u ¹³C束流轰击Be靶, 通过RIBLL选择出丰中子放射性核⁸He. 利用透射法测量了⁸He的去双中子截面和去四中子截面. 利用Ogawa等人的理论结合原有⁸He的反应总截面数据, 得到⁸He的核芯为⁴He的结论.     

中能区丰中子核11Li的反应总截面的测量

利用HIRFL提供的50MeV/u的¹³C束流轰击Be靶, 通过RIBLL选择出放射性核素¹¹Li. 实验采用透射法测量了25—45MeV/u的¹¹Li在²⁸Si靶上的反应总截面. 采用双参数Gauss密度分布形式, 利用Glauber模型很好地拟合了高能和中能区的¹¹Li实验数据, 并从密度分布中提取了核的物质均方根半径.     

轻丰中子核反应中子集团产生截面的理论研究

采用Boltzmann-Langevin方程研究了能量为35MeV/u的¹⁴Be, ⁸He,⁶He,¹¹Li,¹⁷B,¹¹Be,¹⁹C与¹²C靶的反应,计算了产生中子集团的截面, 发现^14,Be与¹²C靶反应产生⁴n的截面与实验值符合得很好. 通过这几个入射核与¹²C靶形成中子集团截面的对比, 发现核的晕中子越多产生中子集团的截面越大, 晕中子数相同时, 质量数越大产生中子集团的截面越大.中子集团可能主要来自晕核子.     

28MeV/u 18O与全阻止厚天然铅靶反应中丰中子汞同位素的截面测量

本次实验利用28MeV/u的¹⁸O束流和一套在线熔化铅靶装置以及4πΔEβ—γ符合技术,测量了该中能重离子反应中丰中子汞同位素^205—208Hg生成的相对截面比以及绝对截面的近似值.并外推出了²⁰⁹Hg的可能生成截面.发现由靶核²⁰⁸Pb削裂两个质子添加一个中子而生成²⁰⁷Hg的截面有一个突然的比较大的下降,这可以由反应的Q值的变化规律得到解释.     

135MeV/u 12C和铁相互作用中靶余核的质量分布

用核化学技术测定了135MeV/u ¹²C和铁相互作用中的靶余核的生成截面,通过高斯电荷分布函数得到了靶余核的质量分布.与46MeV/u ¹²C+Cu相比,发现A<30质量区的产额明显增加,且产物有偏向丰中子一侧的趋势.实验测定的质量分布与熔合碎裂模型和级联两体模型的计算结果进行了比较,结果似乎表明在很高入射能情况下多重碎裂衰变是A<30靶余核生成的主要反应机制.     

25MeV/u 6He在9Be靶上的弹性转移反应研究

报告了25MeV/u ⁶He在⁹Be靶上的弹性散射和弹性转移的实验结果. 用光学模型和一阶DWBA的方法计算了弹性散射和³He集团转移的截面, 计算结果和实验测量基本一致. 计算表明³He在⁹Be中的谱幅度应该明显大于壳模型的理论计算值0.70.     

42MeV/u 12C与115In相互作用的靶余核

使用放射化学方法测定了42MeV/u ¹²C与¹¹⁵In相互作用靶余核的生成截面,得到了质量分布及同位素分布.实验得到的质量分布与使用级联的两体衰变模型GEMINI程序计算的结果很好地相符.根据同位素分布的系统性,对利用中能重离子反应生成新的远离β稳定线的缺中子核素进行了讨论.     

中能8B和9C与Si反应总截面的测量

能量为75MeV/u的¹²C初级束轰击2mm厚的初级Be靶,并利用RIBLL从弹核碎片中分离出54.2MeV/u质子滴线核束8B和61.1MeV/u的⁹C,再轰击Si靶,用透射法测量了它们与Si的反应总截面σ_R.并应用Glauber模型进行理论计算,分析结果表明⁸B和⁹C都可能具有质子晕结构.     

50MeV/u 18O离子轰击Be、Cu和Au厚靶的中子产额和中子发射率

用阈探测器中子活化法测量了50MeV/u ¹⁸O离子轰击Be.Cu和Au厚靶的总中子产额和前向中子发射率. 实验结果表明,中子产额对靶核原子序数有一定的依赖性,较轻靶子的中子产额和中子发射率高于较重的靶子;当靶核(Cu)和入射离子单核能(50MeV)相同时,¹⁸O离子的中子产额约为¹²C离子的4倍.     

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采用了通用高速A/D采集器采集信号数据,用软件的方法开发出了具备多道能谱脉冲识别和计数分析能力的软件.用此软件实现了每次托卡马克放电后,在较短的时间内从庞大的原始采集数据中提取出能谱脉冲数据,计算和显示能谱图,这为下一步测量电子温度打下了基础,并同时实现了数据共享.     

Cross-section measurement of charged-pion photoproduction from hydrogen and deuterium

We have measured the differential cross section for the gamman-->pi(-)p and gammap-->pi(+)n reactions at theta(c.m.)=90 degrees in the photon energy range from 1.1 to 5.5 GeV at Jefferson Lab (JLab). The data at E(gamma) greater, similar 3.3 GeV exhibit a global scaling behavior for both pi(-) and pi(+) photoproduction, consistent with the constituent counting rule and the existing pi(+) photoproduction data. Possible oscillations around the scaling value are suggested by these new data. The data show enhancement in the scaled cross section at a center-of-mass energy near 2.2 GeV. The cross section ratio of exclusive pi(-) to pi(+) photoproduction at high energy is consistent with the prediction based on one-hard-gluon-exchange diagrams.     

Systematics on fission fragment mass distribution of neutron induced 235U fission

Based on the neutron induced fission fragment mass distribution data up to neutron energy 20 MeV measured with the double kinetic energy method (KEM) and the radio active method (RAM), the systematics of fission fragment mass distribution was investigated by using 5 Gaussian model and the systematics parameters were obtained by fitting the experimental data. With the systematics, the yields of any mass A and at any energy in the region from 0 to 20 MeV of neutron energy can be calculated. The calculated results could well reproduce the experimental data measured with KEM, but show some systematical deviation from the data measured by RAM, which reflects some systematical deviations between the two kinds of measured data.The error of systematics yield was calculated in an exact error transformation way, including from the error of the experimental yield data to the error of the discrete parameters, then to the systematics parameters,and at last to the yield calculated with systematics.     

Systematics on fission fragment mass distribution of neutron induced 235U fission

Based on the neutron induced fission fragment mass distribution data up to     

Multiparticle azimuthal correlations in central nucleus-nucleus collisions at high energy

Multiparticle azimuthal correlations in central nucleus-nucleus collisions at high energy are described by a simple formula. The calculated results are in agreement with the experimental data of carbon and oxygen induced interactions at Dubna energy. The comparison between the calculated results and experimental data shows that particles are emitted isotropically in the rest frame of the emission sources, and the emission sources have movements in momentum space.     

Electron energy loss and secondary emission mechanisms in BaO

Electron Loss Spectroscopy (ELS), X-ray Photoemission (XPS), Secondary Emission Energy Distribution, and Secondary Electron yield data have been obtained on both evaporated films and sprayed-on coatings of BaO. Using the ELS correlated with the XPS data, bulk and surface plasmon losses as well as excitonic and interband transition electron loss mechanisms have been identified. It was found that at low primary beam energies (<100 eV), structure in the secondary emission energy distribution could be correlated with a conduction band energy structure. This structure was consistent with the model used to explain the loss transitions. The structure in the energy distribution curves shows little, if any, correlation with plasmon decay mechanisms and other two-step electron emission processes. On the contrary, for the case of BaO (at least at low primary energies), the energy distribution data and structure in the secondary yield vs. primary beam energy data indicate that most secondaries are produced by direct excitation of secondaries by the primary electrons.     

Multiparticle azimuthal correlations in central nucleus-nucleus collisions at high energy

Multiparticle azimuthal correlations in central nucleus-nucleus collisions at high energy are described by a simple formula.The calculated results are in agreement with the experimental data of carbon and oxygen induced interactions at Dubna energy.The comparison between the calculated results and experimental data shows that particles are emitted isotropically in the rest frame of the emission sources,and the emission sources have movements in momentum space.     

Model correction for the formation of amorphous silicon by ion implantation

The critical dose at which an implanted amorphous layer in silicon is formed cannot be explained by a previous energy independent model. An energy dependent correction to this model can explain our ESR data as well as other data. The correction is most important for light ions.     

PSⅡ颗粒二聚体中类胡萝卜素向反应中心传能研究

运用瞬态荧光光谱技术在77 K低温下对PSⅡ颗粒复合物中类胡萝卜素（Car）分子的能量传递过程进行研究, 通过不同激发波长473 nm, 481 nm, 507 nm选择性激发PSⅡ颗粒复合物中色素分子, 得到PSⅡ颗粒二聚体中关于Car能量传递的三组时间组分：16.6 ps, 130~183 ps, 217~249 ps. 其中16.6 ps反映了LHCⅡ中的Car分子将能量通过中间体Cars、Chls分子传递到Chl639的过程; 130~183 ps为核心天线中的β-Car分子向RC的能量传递时间; 217~249 ps为LHCⅡ中Car481通过中间Chla分子向RC的传能时间.