Multi-electron processes in 4.15-11.08 keV/u(13)C(6+) on argon collisions

The relative partial cross sections for C-13(6+)-Ar collisions at 4.15-11.08 keV/u incident energy are measured. The cross-section ratios sigma(2E)/sigma(SC), sigma(3E)/sigma(SC), sigma(4E)/sigma(SC) and sigma(5E)/sigma(SC) are approximately the constants of 0.51 +/- 0.05, 0.20 +/- 0.03, 0.06 +/- 0.03 and 0.02 +/- 0.01 in this region. The significance of the multi-electron process in highly charged ions (HCIs) with argon collisions is demonstrated (sigma(ME)/sigma(SC) as high as 0.79 +/- 0.06). In multi-electron processes, it is shown that transfer ionization is dominant while pure electron capture is weak and negligible. For all reaction channels, the cross-sections are independent of the incident energy in the present energy region, which is in agreement with the static characteristic of classic models, i.e. the molecular Coulomb over-the-barrier model (MCBM), the extended classical over-the-barrier (ECBM) and the semiempirical scaling laws (SL). The result is compared with these classical models and with our previous work of C-13(6+)-Ne collisions

Search for signature inversion in the pi i(13/2)circle times nu i(13/2) bands in Au-182,Au-184,Au-186

Search for low-spin signature inversion in the pi i(13/2) circle times nu i(13/2) bands in odd-odd Au-182,Au-184,Au-186 has been conducted through the standard in-beam gamma-spectroscopy techniques via the Sm-152(Cl-35,5n) Au-182, Yb-172(F-19,5n) (186)An, and Tb-159(Si-29,4n) (184)An reactions, respectively. The pi i(13/2) circle times nu i(13/2) bands in these three nuclei have been identified and extended up to high-spin states. In particular, the inter-band connection between the pi i(13/2) circle times nu i(13/2) band and the ground-state band in Au-184 has been established, leading to a firm spin-and-parity assignment for the pi i(13/2) circle times nu i(13/2) band. The low-spin signature inversion is found in the pi i(13/2) circle times nu i(13/2) bands according to our spin-assignment and-the signature crossing observed at high-spin states.

Low-spin signature inversion in the pi h(9/2)circle times nu i(13/2) oblate band

Excited states in Tl-188,Tl-190 have been studied experimentally by means of in-beam gamma spectroscopy techniques, and resulted in the identification of a strongly coupled band based on the pi h(9/2) circle times nu i(13/2) configuration with oblate deformation. The oblate band in doubly odd Tl nuclei shows low-spin signature inversion. It is the first experimental observation of low-spin signature inversion for a band associated with the oblate pi h(9/2) circle times nu i(13/2) configuration.

Observation of a pi h(9/2) circle times nu i(13/2) oblate band in Tl-188

Excited states in Tl-188 have been studied experimentally using the Gd-157(Cl-35;4n) reaction at a beam energy of 170 MeV. A rotational band built on the pi h(9/2) x nu i(13/2) configuration with oblate deformation has been established for Tl-188. Based on the structure systematics of the oblate pi h(9/2) x nu i(13/2) bands in the heavier odd-odd Tl nuclei, we have tentatively proposed spin values for the new band in Tl-188. The pi h(9/2) x nu i(13/2) oblate band in Tl-188 shows low-spin signature inversion, and it can be interpreted qualitatively by the two-quasiparticle plus rotor model including a J-dependent p-n residual interaction.

Properties of the pi h(9/2)circle times nu i(13/2) oblate band in Tl-188

High spin states in Tl-188 have been investigated via the Gd-157(Cl-35,4n) reaction at beam energy of 170 MeV. A rotational band built on the pi h(9/2) circle times nu(13/2) configuration with oblate deformation has been established. Considering the similarity between the band structure observed in odd-odd Tl nuclei, spin values have been tentatively proposed for the new band in Tl-188. The pi h(9/2) circle times nu(13/2) oblate band in Tl-188 shows low-spin signature inversion, and it can be interpreted qualitatively by the two quasiparticle plus rotor model including a J-dependent p-n residual interaction.

Signature inversion in pi h(9/2) circle times nu i(13/2) oblate band of Tl-188

High-spin Level structure of Tl-188 has been studied via Gd-157 (Cl-35,4n) fusion-evaporation reaction at beam energy of 170MeV. A rotational band built on the pi h(9/2) circle times nu i(13/2) configuration with oblate deformation has been established. Spin values have been proposed to the pi h(9/2) circle times nu i(13/2) oblate band based on the similarities between the oblate band of Tl-188 and those in odd-odd Tl190-200. With the spin assignments, the low-spin signature inversion has been revealed for the pi h(9/2) circle times nu i(13/2) oblate band of Tl-188. The low-spin signature inversion can be interpreted qualitatively in the framework of the quasi-particles plus rotor model including a J dependent p-n residual interaction.

Multi-electron processes in C-13(6+) ions with neon collisions in energy region 4.15-11.08 keV/u

The cross-section ratios of double-, triple-, quadruple-, and the total multi-electron processes to the single electron capture process sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC)) as well as the relative ratios among reaction channels in double-electron active, triple-electron active and quadruple- electron active are measured in C-13(6+) -Ne collision in the energy region of 4.15-11.08 keV/u by employing position-sensitive and time-of-flight coincident techniques. It is determined that the cross-section ratios sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC) are approximately the constants of 0.20 +/- 0.03, 0.16 +/- 0.04, 0.06 +/- 0.02 and 0.42 +/- 0.05. These values are obviously smaller than the predictions of the molecular Coulomb over-the-barrier model (MCBM) [J. Phys. B 23 (1990) 4293], the extended classical over-the-barrier model (ECBM) [J. Phys. B 19 (1986) 2925] and the semiempirical scaling laws (SL) [Phys. Rev. A 54 (1996) 4127]. However, the relative ratios among partial processes of DE, TE and QE are found to depend on collision energy, which suggests that the collision dynamics depends on the collision velocity. The limitation of velocity-independent character of ECBM, MCBM and SL is undoubtedly shown.

2.6 s isomer of Nd-129

Nd-129 was produced by irradiation of an enriched target of Ru-96 with a Ar-36 beam and studied by using a helium-jet fast tape transport system in combination with X-gamma and gamma-gamma coincidence measurements. A 2.6s isomer of Nd-129 was observed for the first time and tentatively proposed to be the configuration of 1/2[411].

X-ray spectrum emitted by the impact of Xe-129(q+) on Mo surface

We studied the characteristic X-ray spectra produced by the interaction of highly charged ions of X-129(q+) (q =25, 26, 27) with surface of metallic Mo. The experimental result shows that highly charged ions can excite the characteristic X-ray spectra of L-shell of Mo when the beam' s intensity is not more than 120 nA. The X-ray yield of single ion reaches a quantitative level of 10(-8) and increases with the increment of the ion' s kinetic energy and ionic charge (potential energy). By measuring the X-ray spectra of Mo-L alpha(1) the M-level lifetime of Mo atom is estimated by using Heisenberg uncertainty relation.

~(129)Xe~(q+)激发Mo表面产生的X射线谱；X-ray spectrum emitted by the impact of ~(129)Xe~(q+) on Mo surface

研究了高电荷态离子129Xeq+(q=25,26,27)入射金属Mo表面产生的特征X射线谱.实验结果表明,在束流强度小于120nA条件下,高电荷态离子129Xeq+可以激发Mo的L壳层特征X射线谱.单离子X射线相对产额可达10-8量级,特征X射线的相对产额随入射离子的动能和电荷态(势能)的增加而增加.通过Mo原子的Lα1特征X射线谱,利用Heisenberg不确定关系对Mo原子的第M能级寿命进行了估算.

3,5-二甲基吡唑对尿素氮转化及NO_3~--N淋溶的影响

采用室内培养和田间试验相结合的方法,探讨了新型硝化抑制剂3,5-二甲基吡唑(DMP)对尿素氮转化及玉米田硝酸盐淋溶损失的影响.结果表明,DMP对尿素水解仅起短暂的抑制作用,但可在较长时间内显著抑制土壤铵的氧化,且随DMP用量的增加,抑制效应显著增强.培养第10 d时,DMP各处理(0.002 5、0.01及0.025 g/kg)的土壤NH4+-N累积量分别比CK提高了5.17、9.36和11.04倍,而NO3--N累积量于培养第14 d时差异最大,与CK相比分别降低了33.30%、61.19%和73.72%(p<0.01).土壤NO2--N只在尿素施用前期有少量累积,但第3 d DMP各处理土壤NO2--N含量降低幅度达95.77%~96.13%;土壤矿质氮总量于10 d以后,随DMP用量的增加,显著降低,而DMP1处理的土壤微生物量N在培养14~56 d期间显著提高.连续2 a的玉米田间试验原位取土测定结果表明,2004和2005年,DMP的施用使作物根系密集层以下(40~100 cm)土层的NO3--N累积总量分别比CK降低了28.77%和44.70%.因此,硝化抑制剂DMP与尿素配合施用是调控氮素转化、缓解氮肥污染的有效措施.

Ajax与WebGIS的集成研究

WebGIS是利用互联网来扩展和完善地理信息系统的一项应用技术,是GIS发展的一个重要方向。Ajax是异步JavaScript和XML技术的组合。本文介绍了地理空间信息网络服务,探讨了Ajax与WebGIS的集成模式,并以Google Maps为例,详细分析了Ajax与WebGIS集成的具体方法。

L-山梨糖还原酶基因在大肠杆菌中的表达及融合蛋白的酶学特性

为获得L 山梨糖还原酶 (SR)整个操纵子序列 ,以 pGEM 3zf(+)作为载体构建了Gluconobactersp .S6基因文库 .结合转化子在以L 山梨糖为唯一碳源培养基上的生长情况 ,利用PCR技术筛选到一个含L 山梨糖还原酶基因的阳性克隆pGEM 3zf(+) sr3/E .coli,酶切鉴定插入片断长度约 5 .0kb左右 .以 pGEM 3zf(+) sr3/E .coli质粒DNA为模板 ,扩增SR结构基因 .PCR产物经测序验证为SR基因序列后 ,与表达载体Pet32a(+)相连 ,转化宿主大肠杆菌AD4 94 (DE3)对SR基因进行表达 ,并利用重金属离子亲和层析技术对SR融合蛋白进行了纯化 ,对其酶学特性进行了研究 .结果表明 :还原型辅酶II(NADPH)是SR酶蛋白的最适电子供体 ;SR酶蛋白的最适反应pH为 7.0 ,pH为6 .5时保持稳定 ,酶活力较高 ;最适反应温度是 5 0℃ ,30℃时热稳定性较好 .SDS PAGE电泳分析 ,SR融合蛋白的Mr 在6 5× 10 3 左右 ,由此推测出天然SR的Mr 在 5 3× 10 3 左右 ,与SR基因序列推测出的分子量大小一致 .图 13表 2参 6

半干旱沙区退耕还林对碳储量和分配格局的影响

以农田和不同退耕还林年限(5、10、15年)的杨树人工林为对象,开展了退耕还林对生态系统有机碳储量和分配格局特征的研究。结果表明:随着退耕年限的增加,生物量碳储量不断积累,且其增加的碳库主要分配在树干。与农田(CK1)相比,退耕还林5年的杨树人工林(Poplar1)0~10、10~20、20~40和40~60cm土壤有机碳含量分别下降了7.65%、36.66%、51.94%和21.4%;退耕还林10年的杨树人工林(Poplar2),不同层次土壤有机碳含量分别提高了69.63%、62.46%、17.07%和66.94%。与农田(CK2)相比退耕还林15年的杨树人工林(Poplar3),0~10、20~40和40~60cm土壤有机碳含量分别提高了31.96%、81.50%和58.05%,而10~20cm土层下降了13.38%。与对照农田相比,5年生杨树人工林0~60cm土壤有机碳储量下降了31%,而10年和15年生杨树人工林土壤有机碳储量分别增加了47%和41%。退耕5年的杨树人工林总的碳储量比对照农田下降了10%,退耕10年和15年的杨树人工林与相应对照农田相比较,生态系统总的碳储量分别提高大约2倍和5倍。说明,农田退耕还林后生态系统碳储量明显增加,增加的碳储量主要积累在地上生物量碳库中。退耕还林初期,土壤有机碳储量表现出下降趋势,随后逐渐恢复甚至高于农田土壤碳储量。