高电荷态离子与Si(110)晶面碰撞的沟道效应研究

不同电荷态低速离子(Arq+,Pbq+)轰击Si(110)晶面,测量不同入射角情况下的次级粒子的产额.通过比较溅射产额与入射角的关系,证实沟道效应的存在.高电荷态离子与Si相互作用产生的沟道效应说明溅射产额主要是由动能碰撞引起的.在小角入射条件下,高电荷态离子能够增大溅射产额.当高电荷态离子以40°—50°入射时,存在势能越高溅射产额越大的势能效应.

热熔合反应合成超重核产生截面的同位素依赖性

通过在形成超重核的重离子俘获和熔合过程中引入位垒分布函数的方法对双核模型做了进一步发展．超重核形成过程中的俘获、熔合和蒸发3个阶段分别采用了半经验的耦合道模型、数值求解主方程和统计蒸发模型的方法来描述．计算了近年来Dubna小组利用热熔合反应48Ca(243Am,3n-5n) 288-286115和48Ca(248Cm,3n-5n)293-291116合成超重新核素的蒸发余核激发函数．系统分析了48Ca轰击锕系元素U,Np,Pu,Am,Cm合成超重核Z=112-116产生截面的同位素依赖性．给出了合成超重新核素最佳的弹靶组合和入射能量,即有最大的超重核产生截面．计算说明,壳修正能和中子分离能是影响超重核生成截面产生同位素依赖性的主要因素．

利用π~-/π~+探测对称能的高密行为

利用同位旋和动量相关的IBUU相对论强子输运模型,以132Sn+124Sn碰撞在E/A=400MeV,b=1fm时为例,研究了在3种不同的对称能作用下发射粒子谱中π-/π+的比率随时间和横动量的演化.计算结果表明,π-/π+的比率与核物质对称能的硬度有一个反向变化关系.由于π介子主要来自于核反应形成的高密区,因此π-/π+的比率可以作为精确研究核物质对称能高密行为的一个探针.通过与实验数据的比较,就能够得出比以往更精确的关于对称能高密行为的重要信息.

强激光场中团簇Na_2的谐波产生

在时间相关的局域密度近似TDLDA理论框架下 ,研究了强激光场中最简单金属团簇Na2 高次谐波的产生。当激光参数选为强度 1.338× 10 12 W/cm2 和频率 5 .2 6 6eV时 ,在激光频率和Na2 的共振频率处成峰 ;而当强度为 5 .0 5 5× 10 12 W/cm2 ,频率为 1.12 4eV时 ,观察到了第三 ,第五次谐波产生。

Isotopic dependence of production cross sections of superheavy nuclei in hot fusion reactions

The dinuclear system model has been further developed by introducing the barrier distribution function method in the process of heavy-ion capture and fusion to synthesize superheavy nuclei. The capture of two colliding nuclei, formation and de-excitation process of compound nucleus are decribed by using empirical coupled channel model, solving master equation numerically and statistical evaporation model, respectively. Within the framework of the dinuclear system model, the fusion-evaporation excitation functions of the systems Ca-48(Am-243, 3n-5n) (288-286)115 and Ca-48(Cm-248, 3n-5n)(293-291)116 are calculated, which are used for synthesizing new superheavy nuclei at Dubna in recent years. Isotopic dependence of production cross sections with double magic nucleus Ca-48 bombarding actinide targets U, Np, Pu, Am, Cm to synthesize superheavy nuclei with charged numbers Z=112-116 is analyzed systematically. Based on these analysis, the optimal projectile-target combination and the optimal excitation energy are proposed. It is shown that shell correction energy and neutron separation energy will play an important role on the isotopic dependence of production cross sections of superheavy nuclei.

Systematics of central heavy ion collisions in the 1A GeV regime

Using the large acceptance apparatus FOPI, we study central collisions in the reactions (energies in A GeV are given in parentheses): Ca-40 + Ca-40 (0.4, 0.6, 0.8, 1.0, 1.5, 1.93), Ni-58 + Ni-58 (0.15, 0.25, 0.4), Ru-96+Ru-96 (0.4, 1.0. 1.5), (96)zr+(96)zr 1.0, 1.5), Xe-129+CsI (0.15, 0.25, 0.4), Au-197 + Au-197 (0.09, 0.12, 0.15, 0.25, 0.4, 0.6, 0.8, 1.0, 1.2, 1.5). The observables include cluster multiplicities, longitudinal and transverse rapidity distributions and stopping, and radial flow. The data are compared to earlier data where possible and to transport model simulations. (C) 2010 Elsevier B.V. All rights reserved.

Thermodynamic study of ibuprofen by adiabatic calorimetry and thermal analysis

Molar heat capacities of ibuprofen were precisely measured with a small sample precision automated adiabatic calorimeter over the temperature range from 80 to 400 K. The polynomial functions of C-p,C-m (J K-1 mol(-1)) versus T were established on the heat capacity measurements by means of the least fitting square method. The functions are as follows: for solid ibuprofen, at the temperature range of 79.105 K less than or equal to T less than or equal to 333.297 K, C-p,C-m = 144.27 + 77.046X + 3.5171X(2) + 10.925X(3) + 11.224X(4), where X = (T - 206.201)/127.096; for liquid ibuprofen, at the temperature range of 353.406 K less than or equal to T less than or equal to 378.785 K, C-p,C-m = 325.79 + 8.9696X - 1.6073X(2) - 1.5145 X-3, where X = (T - 366.095)/12.690. A fusion transition at T = 348.02 K was found from the C-p-T curve. The molar enthalpy and entropy of the fusion transition were determined to be 26.65 kJ mol(-1) and 76.58 J mol(-1) K-1, respectively. The thermodynamic functions on the base of the reference temperature of 298.15 K, (H-T - H-298.15) and (S-T - S-298.15), were derived. Thermal characteristic of ibuprofen was studied by thermo-gravimetric analysis (TG-DTG) and differential scanning calorimeter (DSC). The temperature of fusion, the molar enthalpy and entropy of fusion obtained by DSC were well consistent with those obtained by adiabatic calorimeter. The evaporation process of ibuprofen was investigated further by TG and DTG, and the activation energy of the evaporation process was determined to be 80.3 +/- 1.4 kJ mol(-1). (C) 2003 Elsevier B.V. All rights reserved.

长白山北坡植物群落复杂性的海拔梯度变化(英文)

应用梯度格局法在长白山北坡海拔700m-2600m的坡面上每100 m海拔设置一样地,共计20块样地,通过对同一群落各样方间的相异性测定,对各海拔植物群落的复杂性进行了分析。结果表明,以主林层乔木种的二元数据计算的结果,除亚高山岳桦林外,其它各海拔群落的样方间均表现出较高的相异性,特别是低海拔的阔叶红松林平均相异系数达0.74,明显高于其它植被类型;暗针叶林各群落间差异不大,相对而言1400 m群落样方间的相异性略高于其它群落,表现出过渡性群落树种组成的复杂性;岳桦林树种组成简单,样[(\267\275\274\344\322\262\261\355\317\326\263\366\275\317\270\337\265\304\\317\340\313\306\320\324\241\243)-0.1(\322\324\271\340\304\276\326\326\265\304\266\376\324\252\312\375\276\335\\274\306\313\343\265\304\310\272)]落内的相异性,虽低海拔的阔叶红松林总体上高于其它群落,但差异趋势并不像乔木种那么明显。以各草本植物与所有植物种的二元数据计算的各海拔群落内样方间的相异性,表现出非常相近的趋势,群落内样方间草本植物及所有植物种均以阔叶红松林及高山冻原差异最大,暗针叶林基本稳定于比较相近的水平。图3表1参8。

红松和长白松针叶暗呼吸对连续4个生长季高浓度CO_2处理的响应

以开顶箱法研究了高浓度CO2对长白山两种针叶树—红松和长白松针叶暗呼吸作用的长期影响.对两个树种连续4个生长季进行700和500μmol·mol-1CO2处理,同时设接受大气CO2浓度(约350μmol·mol-1CO2)的开顶箱为对照,在CO2处理的第2,3和4个生长季分别测定了针叶的暗呼吸速率.结果表明:CO2处理的第2个生长季,高浓度CO2下红松和长白松针叶暗呼吸速率增加,可能与碳氮含量变化有关;CO2处理的第3个生长季,高浓度CO2条件下生长的红松针叶暗呼吸速率增加,长白松针叶的暗呼吸速率下降,两树种呈不同响应主要与植株的生长速率不同有关;CO2处理的第4个生长季,红松和长白松针叶的暗呼吸速率均受高浓度CO2抑制.第3个生长季通过改变测量CO2浓度,发现高浓度CO2对长白松针叶暗呼吸作用的短期效应与长期效应呈现一致性,红松不完全相同.红松和长白松针叶的暗呼吸作用对高浓度CO2的响应与CO2处理时间及植株个体的生长发育阶段有关,暗呼吸速率的变化是CO2直接作用与长期驯化共同作用的结果,不能用短期的测定结果预测针叶暗呼吸对高浓度CO2响应的长期效应.