碰撞过程动能损耗的定量分析

使用高速摄像机拍摄碰撞打靶实验中两球的运动过程,使用Tracker视频分析软件对撞球和被撞球的运动轨迹进行分析,得到了整个碰撞过程的具体数据及运动图像,进而定量分析了各个阶段的能量损失.     

p-A Drell-Yan过程中的核效应

利用色偶极模型,在靶静止系中计算了800GeV质子与原子核碰撞的Drell-Yan过程的微分截面,并与E772实验结果进行了比较.结果发现:不考虑能量损失,只计及p-A碰撞中的核遮蔽效应,理论计算就与实验数据甚好符合.     

碰撞打靶实验的设计和探讨

介绍碰撞打靶实验仪在力学实验中的应用     

氢气放电源和X光机X射线源打靶谱的研究

用氢气放电源打靶的方法,测到了系列的谱线.为了鉴别这些谱线,进行了X光机X射线源打靶实验和两种源打靶的对比实验.实验结果表明:在X光机X射线源打靶谱中,除靶材料的特征X射线和两条源谱线外,还存在两种谱线:一种是能量变化的谱线,根据不同衍射角θ和测量角φ的实验结果,及打多晶体靶和非晶体靶的实验事实,表明这种能量变化的谱线是衍射线;另一种是能量恒定不变的谱线.氢气放电源和X光机X射线源打靶谱的对比实验结果表明:两种源打靶谱自洽.这说明和X光机X射线源打靶谱一样,氢气放电源打靶谱中那些能量变化的谱线是衍射线.但     

高能重离子碰撞中心区的粒子密度

在A.Capella等的双链模型的基础上, 讨论了高能重离子碰撞, 特别是对心碰撞时的多重数快度分布, 估算了各种入射能量下, 对心碰撞时中心区能量密度随碰撞核种类的变化. 说明重的重离子在几十GeV能量下的碰撞有可能实现quark-gluon plasma相变的条件.     

模拟计算低能重离子注入彩棉种子的深度(已撤稿)

采用蒙特卡罗方法,模拟计算了20 keV Ti+注入彩棉种子的深度一浓度分布.核碰撞能量损失采用经典的两体碰撞理论,电子能量损失用Lindlaard-Scharff公式,计算得到Ti+在彩棉种子中的最可几深度是6.66μm,与实验结果非常接近.表明理论模型建立相对合理,为研究低能重离子与生物体之间的相互提供了理论基础.     

200GeV/c的质子-核碰撞中产生粒子的多重数分布与能量亏损

我们用多次碰撞模型分析了入射质子动量为200GeV/c的p-Ar和p-Xe碰撞中产生的负粒子的多重数分布. 在与靶核子的每一次碰撞中, 入射粒子损失能量, 损失的能量用于产生粒子的概念在计算中明确考虑, 理论结果与实验符合较好.     

高能p-A碰撞Drell-Yan过程中的初态核效应

核遮蔽和能量损失效应是p-A碰撞中两种重要的初态核效应. 本文利用从轻子-原子核深度非弹性散射实验数据中抽取的束缚核子的部分子分布函数, 在色弦模型中研究了Drell-Yan双轻子对产生过程中的能量损失效应. 通过对FNAL E772和E866实验数据的χ²分析, 得到夸克在冷核中的能量损失率为－dE/dz=2.06GeV/fm. 这和该模型理论预言的结果(－dE/dz～2GeV/fm)一致. 通过将理论计算结果与实验数据进行比较, 发现考虑到能量损失后能很好的解释实验现象.     

球体的对心碰撞问题

碰撞问题是很复杂的,本文谨就力学中的简单情况加以讨论,其目的是说明因碰撞而发生的动量变化和能量变化。碰撞有完全弹性碰撞、非完全弹性碰撞及完全非弹性碰撞三种情况。如两物体碰撞后没有残留变形,机械能能有损失,则称这样的碰撞为完全弹性碰撞(这是理想情况)。     

浅论Kane难题

文章研究了刚性球壳与固定的刚性水平面的碰撞,在动能损失计算式中引入了碰撞点的切向末速度与切向初速度之比,根据能量守恒定律指出了合理的k值范围,从而指出了Kane难题即碰撞过程中的动能损失小于零的原因。     

Xe~(26+)入射Au靶离子L壳层空穴的产生与退激辐射

基于两体碰撞过程的能量与角动量守恒,推导出Xe26+离子与Au原子碰撞过程,单离子的L壳层空穴产额与离子动能的理论关系.实验测定了动能2.4-3.6Me V的Xe26+离子入射Au靶,产生的Xe的L-X射线谱,获得了射线产额与离子入射动能的实验关系.结果表明,碰撞过程产生Xe L壳层空穴的同时,产生了一定数目的 M壳层空穴,导致L壳层空穴平均荧光产额显著变大,在实验能量范围,空穴产额的理论值与射线产额的实验值存在较好的一致性.     

Baryon-Baryon correlations at small relative momentum in Neon- and Argon-nucleus collisions betweenE/A=200 and 1000 MeV

Two-proton correlation functions at small relative momentum have been systematically studied with the large solid angle detector DIOGENE at Saturne for interactions induced by Ne and Ar beams on various targets, and incident energies per nucleon ranging from 200 to 1000 MeV. From these distributions, informations on the space-time structure of the source have been derived as a function of the centrality of the collision, the target-projectile combinations and the incident energy, using the model of Koonin. Special attention has been devoted to take into account all experimental biases in order to get the distorted theoretical correlation curves before comparison to the experimental data. Other interesting conclusions have been obtained when comparing the extracted source radii to the dimensions of the overlapping volume of target by projectile in a pure geometrical model of the collision (clean cut geometry). Some results concerning fragment-fragment small angle correlations are also presented.     

Energy loss of light ions in metals

On the basis of dielectric formalism the analytical expressions for the calculation of close collision and plasmon excitation contributions to the total energy loss of light ions (protons, α-particles) on valence electrons of metals have been obtained. The importance of accounting for the relation between the mentioned contributions while interpreting the results on ion dechannelling due to their multiple scattering on the crystal valence electrons has been pointed out. The ratio of the total energy loss for the best channelled light ions to the energy loss in the non- oriented target in the energy range of E ≈ 100 keV-500 MeV has been calculated.     

Entrance channel effects on preequilibrium emission and incomplete fusion in Promptly Emitted Particle model

In intermediate energy heavy ion collision prompt particles emitted in the early stages of the reaction affect the properties of the incompletely fused composite. We have studied the entrance channel effects on preequilibrium proton emission and various observables, like temperature, residual velocity, and linear momentum transfer of the incompletely fused residue, in the framework of Promptly Emitted Particle (PEP) model. The calculated preequilibrium proton energy spectra for Oxygen and Sulphur induced reactions on various targets have been confronted with the respective experimental data and the agreement between the two has been found to be quite satisfactory. Proton multiplicity has been found to decrease/increase with the increase in target/projectile mass. Residual velocity and linear momentum transfer have been found to have weak dependance on target mass. With the increase in incident energy, the calculation predicts a tendency towards limiting the temperature of the residue for all the target masses. The limiting temperature has been found to decrease with increase in the mass of the residue which is in accordance with the experimental observations.One of the authors (S.D) is thankful to R. Auble and his collaborators at Oak Ridge National Laboratory, for providing the experimental data. The authors would also like to thank Dr. S.K. Basu for his help in running the code PACE2.     

15eV的质子与羟基碰撞的动力学

采用含时密度泛函理论和分子动力学非绝热自洽耦合的方法,全微观研究沿垂直羟基分子轴向入射初动能为15 eV的质子与羟基碰撞过程的电子-离子关联动力学.计算质子和羟基动能、碰撞后羟基电子和离子的运动状态及系统电子密度的实时分布.结果表明:质子与羟基碰撞后俘获羟基的一部分电子被反弹并损失26.7%的初始动能而羟基动能增加.碰撞后丢失1%电子的羟基在保持碰撞前收缩振动的同时向计算边界平动并以93%的中性和7%的+1价的几率存在.     

6 MeV/u 的19F+27Al 反应碎片的发射机制

重离子核反应中的碎片发射机制是近年来人们十分关注的研究课题。利用ΔE-E 探测器,测量了~6 MeV/u 的19F+27Al 反应中核电荷数Z = 2 ~13 的出射碎片。对产物的能谱、角分布、激发函数及能量自关联函数的分析表明,出射产物主要来自弹靶核深部非弹性碰撞所形成的转动的双核系统。In recent years, extensive studies have been made to understand the fragment emission mechanisms in low energy light heavy-ion reactions. These fragments are found to be emitted from quasielastic/projectile breakup, deep-inelastic and fusion-fission processes. Fragments of Z = 2~13 induced by the collision of 19F+27Al have been measured by ΔE-E telescope. The analysis of the energy spectra, angular distributions, excitation functions and energy auto-correlation functions of these fragments shows that the emission of fragments is coming from a rotational dinuclear system formed in the dissipative collision of the projectile and target nuclei.     

多功能球-球碰撞实验仪的研制

研制了多功能球-球碰撞实验仪,利用该仪器对三组碰撞实验的研究发现,未退火小球和未退火小球碰撞可近似为弹性碰撞,其恢复系数为0.96;未退火小球和退火小球、退火小球和退火小球之间的碰撞为非弹性碰撞。本实验源自生活中的打靶实验,将其进行改造升级为物理实验中的研究性设计性实验,在启发学生创新思维和培养学生发散思考方面具有显著作用。     

电子碰撞Ne和类Ne离子电离的三重微分截面理论研究

采用扭曲波玻恩近似理论计算了共面对称几何条件下类Ne离子2p轨道电子在不同出射电子能量下的(e,2e)反应三重微分截面,出射电子能量分别为3,5,7.5,10,15,20,30和50 eV.计算结果表明,随着出射电子能量的增大和核电荷数Z的增大,三重微分截面的幅度逐渐减小.除Ne以外,对其他离子,在出射电子角度为150?附近出现了一个新的结构,对比不同出射电子能量时的(e,2e)反应三重微分截面,发现这个结构的幅度随着出射电子的能量先增大后减小,文中用一种两次两体碰撞过程对这些现象进行了解释.     

Multiquantum scattering processes and transmission electron energy loss spectra

Microscopic many-body theory for electronic properties of solid states is developed with an emphasis on the role of correlation memory effects. Heisenberg equation of motion, fluctuation-dissipation theorem and operators of commutation have been used to calculate multiplasmon transmission electron energy loss spectra. Multiquantum integral kinetic equation for the longitudinal complex dielectric function is derived. Strong interaction between high-energy probe beam electrons penetrating the solid state and plasma of valence electrons is taken into account. It is shown that average number of high-frequency plasmons generated in every collision process is more than one for typical values of metal parameters. It is obtained that excitation of a good few plasmons is simultaneous event. Calculated multiplasmon structure of electron energy loss spectra coincides with experimental.