Large Decay Rate Variation of ^7Be in Pd and Au

Platinum and gold have the similar crystal structure but different electronic affinities, as well as different effective electron densities near the implanted ions. Both the differences favour larger decay rate of ^7 Be in Pd than that in Au. We measured the variation of the decay rate of ^7Be implanted in Pd and Au host materials. We have found that the decay rate of ^7 Be in Pd is larger than that in Au by 0.8%.     

试用特洛伊木马方法研究天体核反应9Be（p，α）6Li

为克服低能带电粒子核反应截面直接测量中所遇到的库仑位垒和电子屏蔽效应带来的困难，试用基于准自由反应机制的特洛伊木马方法，在意大利南部国家核物理实验室的15MV串列加速器上，通过^2H（^9Be，α^6Li）n核反应对^9Be（p，α）^6Li在低能区（Ecm=0-1000kev）的裸核反应截面做了间接测量，并将测量结果与直接测量数据进行了比较。The beryllium abundance acts as a key role for understanding the inhomogeneous Big Bang nucleosynthesis. In order to measure the ^9Be（p, α）^6Li bare nucleus cross section and S（E） factor at astrophysical energies, the Trojan Horse Method （THM） can be applied. The main feature of the method is that it allows to extract the energy dependence for the astrophysical S（E） factor of bare nuclei at very low energies without any extrapolation, by measuring the cross section of an appropriate three body process. Thus the ^9Be （p,α）^6Li has been studied by means of the THM applied to the ^2H（^9Be,α^6Li）n at INFN-LNS, Catania, Italy. The two body reaction cross section has been studied in the energy range of Ecm=0-1 000 keV. Preliminary results are discussed and a comparison with direct data is made.     

Measurement of Change of ^7Be Decay Rate in Be and Au

We have measured the possible change of the decay rate of ^7Be implanted into hosts of natural beryllium and natural gold. No difference between the ^7 Be decay rates in the two hosts is observed within the experimental precision of 0.12%. This result implies that change of the decay rate of ^7Be implanted in different materials cannot be simply expected from the electron affinity difference consideration lonely and the lattice structure of the host materials should be taken into account.     

90Mo电磁跃迁几率的测量

利用束流能量为116MeV的⁵⁹Co(³⁵Cl,2p2n)⁹⁰Mo反应布居⁹⁰Mo的高自旋态.用10台反康普顿HPGe探测器组成的探测阵列进行γγ符合测量.通过多普勒展宽峰的形状分析测定⁹⁰Mo高自旋态的寿命.在正宇称衰变系观察到增强的M1跃迁,推断I=13以上是扁椭形变.负宇称高自旋态具有大的B(E2)值,并随自旋增大而起伏变化.正、负宇称态之间的跃迁显示增大的E1跃迁,似有八极关联的可能.但是,⁹⁰Mo并不处在理论预言的存在八极形变的核区内.     

氢硼聚变三体级联衰变连续能谱的Monte-Carlo模拟与分析

¹¹B(p,α1)⁸Be^*(1)(2α)三体级联衰变中居间核8Be⁽¹⁾衰变成两个α粒子的连续能谱呈马鞍形分布.编写了模拟三体级联衰变连续能谱的Monte-Carlo程序,计算结果表明:沿居间核8Be⁽¹⁾运动方向α发射强度增强的各向异性分布,能较好地解释实验结果,揭示p+¹¹B核反应中⁸Be⁽¹⁾核α衰变各向异性发射.     

特洛伊木马方法及其应用最新进展

特洛伊木马方法是实验核天体物理中一种重要的间接测量方法，特别适合极低能区带电粒子裸核反应截面测量。在介绍特洛伊木马方法基本原理的基础上，重点讨论该方法近期在核天体物理应用中的一些重要实验结果，以及对未来研究的展望。主要介绍:AGB星s-过程关键中子源反应$ ^{{\rm{13}}}{\rm{C(\alpha ,n}}{{\rm{)}}^{{\rm{16}}}}{\rm{O}}$的间接测量，AGB星氟丰度超常现象相关核反应间接测量，以及最近热点–中等以上质量恒星碳燃烧核反应间接测量结果及相关争议。     

Geant4模拟在特洛伊木马方法中的应用

由于低能带电粒子核反应截面直接测量遇到的库仑位垒和电子屏蔽势的困难,基于准自由反应机制的特洛伊木马方法得到特别关注。利用Geant4模拟的结果,与在中国原子能研究院串列加速器上通过三体反应9Be+2H→8Be+2H+n对两体反应9Be+1H→8Be+2H的反应截面做的间接测量实验数据进行了比较,这是Geant4模拟在特洛伊木马方法中的首次应用。通过对模拟数据研究,提高了对实验数据的理解,也检验了模拟系统的可靠性,对今后的实验设计和改进提供了有益的意见。     

低能离子注入育种中次级效应影响的模拟研究

低能离子注入育种作为一种有效的育种方法在实践中进行了大量的尝试并取得了一系列重要成果,但其作用机理一直都存在着巨大的争议,特别是射程很短的低能重离子如何穿透到种子内部触发生物效应。本研究利用SRIM、CASINO、Geant4模拟程序对低能离子注入生物样品的离子注入深度进行模拟和定量分析,并对次级粒子可能产生的影响进行了定量模拟研究。结果显示,低能重离子本身射程一般都小于1 μm,选用轻离子、提高注入能量、采用干种子进行注入,都有利于增加穿透深度。次级过程中,反冲质子的最大射程比初级入射离子的稍大,不能显著提升穿透能力。次级过程产生的粒子中只有X射线可以明显提高穿透种子的深度,只要剂量足够大,总会有少量X射线穿透到很深的地方。The breeding method by low-energy ion implantation has been proved to be a valuable breeding method by a large number of practical attempts, but the mechanism of the method has always been in a large dispute. The most difficult thing to be understood is how the low energy heavy ion with such a short range (normally shorter than 1 μm) can penetrate into the inner part of seeds to trigger the biological effects. In this paper, simulations with quantitative analysis were performed for the low energy ion implantating into biological samples and the effects caused by the secondary particles using SRIM, CASINO and Geant4 simulation programs. The results showed that the ranges of low energy heavy ions are normally less than 1 μm. The ranges can become longer if dry seeds and light ions are used with a higher energy. The ranges of recoil protons are only a little longer than that of the primary ions. Among the secondary particles produced in the ion implanting process, only the X-ray can obviously increase the penetration depth in seeds. There always will be a small amount of X-rays which can penetrate into the deeper place in the seed if the ion dose is high enough.     

Influence of particle packing structure on sound velocity

The anisotropy in the particle systems of different packing structures affects the sound velocity. The acoustic propagation process in four kinds of packing structures(denoted as S45, H60, S90, and D) of two-dimensional granular system is simulated by the discrete element method. The velocity v_(tof) obtained by the time of flight method and the velocity vc obtained from the stiffness tensor of the system are compared. Different sound velocities reflect various packing structures and force distributions within the system. The compression wave velocities of H60 and S90 are nearly the same, and transmit faster than that of D packing structure, while the sound velocity of S45 is the smallest. The shear wave velocities of S45 and H60 are nearly the same, and transmit faster than that of D packing structure. The compression wave velocity is sensitive to the volume fraction of the structure, however, the shear wave velocity is more sensitive to the geometrical structure itself. As the normal stress p is larger than 1 MPa, v_(tof) and vc are almost equal, and the stiffness tensors of various structures explain the difference of sound velocities. When the normal stress is less than 1 MPa, with the coordination number unchanged, the law v_(tof) ∝ p~(1/4) still exists. This demonstrates that apart from different power laws between force and deformation as well as the change of the coordination number under different stresses, there are other complicated causes of v_(tof)∝ p~(1/4), and an explanation of the deviation from v_(tof) ∝ p~(1/6) is given from the perspective of dissipation.     

7Be在Pd和Au中衰变率变化的相对测量

将HI-13串列加速器次级束流线产生的放射性核素7Be分别注入到Pd和Au中,利用两个高纯锗探测器同时测量7Be EC衰变核素7Li第一激发态放出的478 keV γ射线产额随时间的变化,发现7Be在Pd中的衰变率比在Au中大(0.8±0.2)%,并讨论了衰变率差别与这两种材料的电子亲合势及有效电子密度的关系.