全永磁ECR离子源研究进展

ECR(电子回旋共振)离子源是产生稳定的强流多电荷态离子束流最有效装置。全永磁ECR离子源因其独特的特点为很多中小型多电荷态离子束流实验平台与离子注入机等系统所采用,为后者产生重复性好、稳定性强的多电荷态离子束流。本文着重论述了中国科学院近代物理研究所研制的几台全永磁多电荷态ECR离子源及其特性与典型性能,如能产生强流高电荷态离子束流的高性能全永磁离子源LAPECR2,能产生强流中低电荷态离子束流的LAPECR1,能产生多电荷态重金属离子束流的LAPECR1-M等。这些性能稳定的离子源为提高近代物理研究所相关试验平台的性能提供了关键的束流品质保障。

Synchronism of Holocene East Asian monsoon variations and North Atlantic drift-ice tracers (vol 65；pg 443；2006)

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两种位置灵敏平行板雪崩探测器

为兰州重离子加速器放射性次级束流线 (RIBLL)设计研制了两种结构双维位置灵敏低压气体平行板雪崩探测器 (PPAC)。用 3组分α粒子辐照 ,传统结构的PPAC ,对于 70 0Pa异丁烷和C3F8工作气体 ,分别得到 0 76mm(FWHM )和 0 64mm(FWHM)的位置分辨 ,探测效率为 99 1 %。新的多级位置灵敏平行板雪崩探测器 (MPPAC) ,对 65 0Pa异丁烷工作气体 ,测得 0 5 8mm (FWHM )的位置分辨、99 2 %探测效率和色散远好于± 0 2mm的位置线性。MPPAC增益较传统PPAC高 ,C3F8较异丁烷阻止本领强 ,适合探测较轻粒子。

太白山古冰川遗迹资源与旅游可持续开发

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分布式控制系统中设备服务器软件的设计与实现

讲述了分布式控制系统中用于提供设备访问服务的设备服务器软件的实现方法。详细介绍了多线程网络通信的设计与实现方法，并对软件中的多线程同步、日志维护、数据库操作等问题进行了讨论。

探测丰中子核弱γ活性的符合反符合系统

HPGeγ探测器的γ射线能量信号与 4πΔEβ 探测器的 β射线能损信号相符合 ,再与大的BGO探测的正电子湮灭 5 11keVγ射线信号作反符合 ,由此构成的特殊探测系统在新丰中子核素2 0 9Hg的首次观察中起到了重要作用 ,显示出对从元素分离的样品中探测非常弱的丰中子同位素γ活性是一种很有效的方法

轻粒子发射时间随测量角的变化

利用小相对角关联方法测量了 2 5MeV u40 Ar+ 93Nb反应中关联出射的轻粒子 .通过与三体弹道模型的比较 ,从关联函数提取了轻粒子的发射时间 .结果表明 ,轻粒子的发射时间随粒子能量的升高而降低 ,从低能的约 60 0fm c下降至高能的约 50fm c .将此数据与40 Ar+ 1 97Au反应中的发射时间进行了比较 ,发现随着实验室系角度的增加 ,提取的轻粒子的发射时间变长 ,并认为其原因在于随发射角度的增加 ,前平衡发射成份越来越少 ,平衡发射成份增加

用~(12)C离子模拟质子引起的单粒子效应

在理论分析的基础上 ,提出了一种利用兰州重离子加速器提供的高能 12 C离子模拟质子引起单粒子效应的途径 .在保证核反应机制是引起单粒子效应主要机制的前提下 ,用高能 12 C离子可以模拟质子在功率金属 -氧化物 -半导体场效应晶体管中引起的单粒子烧毁以及单粒子栅极击穿 ,获得质子单粒子效应的饱和截面 ,定性研究质子单粒子效应的角度效应 ,还可以作为高能质子单粒子效应实验前的预备实验 .该方法拓展了兰州重离子加速器加速的轻的重离子在单粒子效应实验研究方面的应用 ,对现阶段国内开展质子单粒子效应实验研究具有重要意义

~(19)F+~(93)Nb重离子耗散碰撞中截面测量的不可重复性(英文)

完成了１９Ｆ＋９３Ｎｂ重离子耗散碰撞激发函数的两次独立测量．束流１９Ｆ８＋的入射能量１００—１０８ＭｅＶ，能量步长２５０ｋｅＶ；两次测量中分别使用了厚度为７０和７１μｇ／ｃｍ２的９３Ｎｂ靶，其它宏观实验条件（例如，入射能量及能量步长，探测器及其探测角度，加速器、电子学以及数据获取系统的参数选取等等）则保持完全相同．实验结果表明，两次测量所得到的耗散产物截面的激发函数的不平滑结构具有不可重复性．这一实验结果支持了最近提出的理论预言：“在复杂量子碰撞中存在对初始条件的极端敏感性与混沌运动．”

High-spin structure in Pt-187

High-spin states in Pt-187 were studied via the Yb-173(O-18, 4n) reaction. Rotational bands based on the vi(13/2), v7/2(-)[503], vi(13/2)(2)vj, v3/2(-)[512] and v1/2(-)[521] configurations were observed, and interpreted within the framework of the cranked shell model. The TRS calculations show that the vi(13/2) band has an appreciable negative gamma deformation, and the negative-parity bands tend to have a near prolate shape with small positive gamma values. Experimental values of B(M1)/B(E2) ratios have been extracted and compared with theoretical values from the semi-classical Donau and Frauendof approach, strongly suggesting a low frequency pi h(9/2) alignment in the v7/2(-)[503] band.

Band properties of the transitional nucleus Pt-187

High-spin states in Pt-187 have been studied experimentally using the Yb-173(O-18, 4n) reaction at beam energies of 78 and 85 MeV. The previously known bands based on the nu i(13/2),nu 7/2(-)[503], and nu i(13/2)(2)nu j configurations have been extended to high-spin states, and new rotational bands associated with the nu 3/2(-)[512] and nu 1/2(-)[521] Nilsson orbits have been identified. The total Routhian surface calculations indicate that the transitional nucleus Pt-187 is very soft with respect to beta and gamma deformations. The band properties, such as level spacings, band crossing frequencies, alignment gains, and signature splittings, have been compared with the systematics observed in neighboring nuclei and have been interpreted within the framework of the cranked shell model. The rotational bands show different band crossing frequencies, which can be explained by the alignment either of i(13/2) neutrons or of h(9/2) protons. Importantly, evidence is presented for a pi h(9/2) alignment at very low frequency in the nu 7/2(-)[503] band. The proton nature of the band crossing is strongly suggested by comparing the measured B(M1;I -> I-1)/B(E2;I -> I-2) ratios with the theoretical values from the semiclassical Donau and Frauendof approach.

Quasiparticle nature of rotational bands in Pt-187

The high-spin states in Pt-187 have been studied experimentally by means of in-beam gamma-ray spectroscopy techniques via the Yb-173(O-18, 4n) fusion-evaporation reaction. The high-spin level scheme of Pt-187 has been established, including three rotational bands. Based on the systematics of level structure in neighboring nuclei and by comparing the experimental and theoretical B(M1)/B(E2) ratios, configurations of 11/2+ [615], 7/2(-)[5031 and 1/2(-)[521] have been proposed for the three rotational bands, respectively. Band properties of band crossing frequency, alignment gain and signature splitting have been discussed.

Study of quasiparticles bands in odd-odd Au-188

High-spin level structure of Au-188 has been studied via the Yb-173(F-19, 4n gamma) reaction using techniques of in-beam gamma-ray spectroscopy. Based on the experimental results, the level scheme of 188Au has been revised significantly. The previously reported positive parity levels have been modified and a new 20(+) level was proposed to feed the 18(+) states via two low-energy transitions. The existence of the 20(+) and the level structures above it are similar to those in the neighboring odd-odd Au-190,Au-192, therefore, the pi h(11/12)(-1)circle times-vi(13/2)(-2)h(9/2)(-1) configuration was assigned to the 20(+) state.