Characteristics of indoor/outdoor PM2.5 and elemental components in generic urban；roadside and industrial plant areas of Guangzhou City；China

IEECAS SKLLQG

A 10,000 year record of dune activity；dust storms；and severe drought in the central Great Plains

IEECAS SKLLQG

陕西关中东部不同土地利用方式下土壤元素的剖面分布特征

IEECAS SKLLQG

陕西省主要城市工业废气污染现状及防治措施

IEECAS SKLLQG

Seasonal precipitation in the south-central Helan Mountain region, China, reconstructed from tree-ring width for the past 224 years

IEECAS SKLLQG

区域资源环境系统物质流动模式

IEECAS SKLLQG

Isospin diffusion and equilibration for Sn plus Sn collisions at E/A=35 MeV

Equilibration and equilibration rates have been measured by colliding Sn nuclei with different isospin asymmetries at beam energies of E/A = 35 MeV. Using the yields of mirror nuclei of Li-7 and Be-7, we have studied the diffusion of isospin asymmetry by combining data from asymmetric Sn-112 + Sn-124 and Sn-124 + Sn-112 collisions with those from symmetric Sn-112 + Sn-112 and Sn-124 + Sn-124 collisions. We use these measurements to probe isospin equilibration in central collisions where nucleon-nucleon collisions are strongly blocked by the Pauli exclusion principle. The results are consistent with transport theoretical calculations that predict a degree of transparency in these collisions, but inconsistent with the emission of intermediate mass fragments by a single chemically equilibrated source. Comparisons with quantum molecular dynamics calculations are consistent with results obtained at higher incident energies that provide constraints on the density dependence of the symmetry energy.

高电荷态238Uq+在碳膜中电荷平衡时间的研究

离子通过物质过程中与靶原子发生碰撞，碰撞中大量电子被俘获和电离。当电子俘获截面与电离截面达到平衡时，出射离子的电荷态分布达到一个平衡的分布，这个分布与入射离子的核电荷数、速度、壳层结构以及靶材料的性质有关。研究离子通过物质后的电荷态分布和电荷平衡时间对于研究高电荷态离子穿越物质层时的电荷转换及平衡过程具有重要意义。 本文论述了能量为0.8 MeV/u 238Uq+离子通过不同厚度碳膜后的电荷态分布，并对铀离子在碳膜中的电荷平衡时间进行了研究。 实验中束流采用兰州重离子加速器国家重点实验室（HIRFL）首次加速出的能量为0.8 MeV/u 238U26+离子束。本实验是首次在兰州放射性次级束流线（RIBLL）实验终端进行，采用的实验方法新颖。为了研究不同初始电荷态的铀离子通过不同厚度碳膜后的电荷态分布，实验中采取让初级束流 238U26+通过0.1µm厚度碳膜后形成一个电荷态分布，通过调节二极磁铁的控制电流从中选择某一电荷态轰击碳靶，进行电荷态分布研究。 实验对0.8 MeV/u 238Uq+(q=26，29，34，39)通过不同厚度碳膜（5µg/cm2，15µg/cm2，26µg/cm2和225µg/cm2）后的电荷态分布进行了研究。结果发现：能量为0.8 MeV/u的铀离子通过5µg/cm2厚度碳膜后，出射铀离子的电荷态分布未达到平衡；同样铀离子通过15µg/cm2厚度碳膜后，出射铀离子的电荷态分布已达到平衡，平衡平均电荷态为33.72+；由此通过计算得到铀离子在碳膜中的电荷平衡时间为1/3×5.4fs<=t<=5.4fs