Group Invariant Solutions of the Plastic Torsion of Rod with Variable Cross Section

Based on the theory of Lie group analysis, the full plastic torsion of rod with arbitrary shaped cross sections that consists in the equilibrium equation and the non-linear Saint Venant-Mises yield criterion is studied. Full symmetry group admitted by the equilibrium equation and the yield criterion is a finitely generated Lie group with ten parameters. Several subgroups of the full symmetry group are used to generate invariants and group invariant solutions. Moreover, physical explanations of each group invariant solution are discussed by all appropriate transformations. The methodology and solution techniques used belong to the analytical realm.     

材料二次电子产额对腔体双边二次电子倍增的影响

采用蒙特卡罗抽样与粒子模拟相结合的方法,数值研究了材料二次电子产额对腔体双边二次电子倍增瞬态演化及饱和特性的影响.研究发现:随着材料二次电子产额的增加,二次电子增长率以及稳态二次电子数目和振幅均呈现增加的趋势,放电电流起振时间逐步缩短,稳态电流幅值以及放电功率平均值和振幅值均呈现逐步增加并趋于饱和的规律,沉积功率波形延时以及脉宽呈现逐步增加并趋于饱和的趋势.粒子模拟给出了高/低二次电子产额情况下的电子相空间分布、电荷密度分布、平均碰撞能量、平均二次电子产额、二次电子数目和放电电流的细致物理图像.模拟结果表明:高二次电子产额材料,饱和时更倾向趋于单边二次电子倍增类型分布;低二次电子产额材料的二次电子倍增饱和特性由空间电荷场的"去群聚"效应和"反场"效应同时决定,而高二次电子产额材料的二次电子倍增饱和特性则主要是由发射面附近的强空间电荷场"反场"效应决定的.     

介质部分填充平行平板传输线微放电过程分析

本文主要研究了介质填充微波部件微放电随时间演变的过程,重点分析了介质微波部件微放电自熄灭机理.以介质部分填充平行平板传输线为研究对象,忽略空间电荷效应,采用自主研发粒子模拟软件模拟微放电过程,并将模拟结果与金属微波部件结果进行对比.结果表明,在一定功率下,金属微放电过程中电子数目呈指数形式增长,而介质微放电过程经历初始电子倍增后发生自熄灭现象,同时发现在电子数目即将下降为0时,介质表面的平均二次电子发射系数大于1或约等于1.另外,在上述模拟结果的基础上对微放电过程中介质表面积累电荷问题进一步分析,模拟结果表明,如果持续向微波部件内注入电子,介质表面的平均二次电子发射系数最终都约等于1.所得结论对研究复杂介质填充微波部件微放电的机理具有一定的理论指导价值.     

强爆炸光辐射脉冲辐照特征与爆炸当量的相关性

为定量分析强爆炸光辐射辐照特征及其与爆炸当量的关系,建立了用于描述光辐射输运过程的辐射流体力学模型。在算子分裂方法运用的基础上,采用温度梯度作为指示子进行并行区域的动态划分,从而实现较高效率的并行求解。在此基础上数值计算了千吨~兆吨当量下强爆炸光辐射的发展过程,分析表明:光辐射强度随时间呈现“双脉冲”变化,强度极小和强度第2极大时刻与当量的某次方成正比。光辐射总功率变化历程与光辐射强度变化历程相似,但受辐射源半径随当量变化的影响,其极值时刻会出现差异。     

Preliminary test results of LAr prototype detector

Liquid argon (LAr) is an attractive target for the direct detection of WIMPs. A LAr prototype detector was designed to study the technology and properties of LAr detectors. The prototype detector had an active volume containing 0.65 kg of liquid argon. A liquid nitrogen (LN) cooling system allowed the temperature fluctuation of the liquid argon to be controlled within less than 0.1 K during a one month run. In the ²²Na calibration run, the LAr prototype obtained 1.59±0.02 p.e./keV light yield for 511 keV gamma rays using a domestic-made argon purification system.     

Secondary electron emission characteristics of graphene films with copper substrate

For modern and future circular accelerators, especially high-intensity proton synchrotrons or colliders, the electron cloud effect is a key issue. So, in order to reduce the electron cloud effect, exploring very low secondary electron yield (SEY) material or coating used in vacuum tubes becomes necessary. In this article, we studied the SEY characteristics of graphene films with different thicknesses which were deposited on copper substrates using chemical vapor deposition. The SEY tests were done at temperatures of 25℃ and vacuum pressure of (2-6)×10^-9 torr. The properties of the deposited graphene films were investigated by X-ray photoelectron spectroscopy (XPS) and Raman spectroscopy. The SEY curves show that the number of graphene layers has a great effect on the SEY of graphene films. The maximum SEY of graphene films decreases with the increase of the number of layers. The maximum SEY of 6-8 layers of graphene film is 1.25. These results have a great significance for next-generation particle accelerators.     

Study on the temperature dependence of BGO light yield

The temperature dependence of BGO coupled with photomultiplier tube R5610A-01 was studied in the range of-30–30℃. The temperature coefficient of the BGO and R5610 A as a whole was tested to be-1.82%/℃. And the temperature coefficient of the gain of the R5610 A is-0.44%/℃ which was tested in the same situation using a blue LED. Thus the temperature coefficient of BGO's light yield can be evaluated as-1.38%/℃.     

Measuring partial fluorescence yield using filtered detectors

Typically, X‐ray absorption near‐edge structure measurements aim to probe the linear attenuation coefficient. These measurements are often carried out using partial fluorescence yield techniques that rely on detectors having photon energy discrimination improving the sensitivity and the signal‐to‐background ratio of the measured spectra. However, measuring the partial fluorescence yield in the soft X‐ray regime with reasonable efficiency requires solid‐state detectors, which have limitations due to the inherent dead‐time while measuring. Alternatively, many of the available detectors that are not energy dispersive do not suffer from photon count rate limitations. A filter placed in front of one of these detectors will make the energy‐dependent efficiency non‐linear, thereby changing the responsivity of the detector. It is shown that using an array of filtered X‐ray detectors is a viable method for measuring soft X‐ray partial fluorescence yield spectra without dead‐time. The feasibility of this technique is further demonstrated using α‐Fe₂O₃ as an example and it is shown that this detector technology could vastly improve the photon collection efficiency at synchrotrons and that these detectors will allow experiments to be completed with a much lower photon flux reducing X‐ray‐induced damage.     

Water‐Dispersible Silicon‐Quantum‐Dot‐Containing Micelles Self‐Assembled from an Amphiphilic Polymer

The dispersion of silicon quantum dots (Si QDs) in water has not been established as well as that in organic solvents. It is now demonstrated that the excellent dispersion of Si QDs in water with photoluminescence (PL) quantum yields (QYs) comparable to those for hydrophobic Si QDs can be realized by combining the processes of hydrosilylation and self‐assembly. Hydrogen‐passivated Si QDs are initially hydrosilylated with 1‐dodecence. The toluene solution of the resulting dodecyl‐passivated Si QDs is mixed with the water solution of the amphiphilic polymer of Pluronic F127 to form an emulsion. Dodecyl‐passivated Si QDs are encapsulated in the micelles self‐assembled from F127 in the emulsion. The size of the Si‐QD‐containing micelles may be tuned in the range from 10 to 100 nm. Although self‐assembly in the emulsion causes the PL QY of Si QDs to decrease, after a few days of storage in ambient conditions, Si QDs encapsulated in the water‐dispersible micelles exhibit recovered PL QYs of ≈24% at the PL wavelength of ≈680 nm. The intensity of the PL from Si QDs encapsulated in the water‐dispersible micelles is >90% of the original value after 60 min ultraviolet illumination, indicating excellent photostability.     

芴酮引发光接枝改性LDPE膜的研究

采用紫外光引发接枝表面改性的方法,以芴酮(FL)为引发剂,在低密度聚乙烯(LDPE)薄膜表面上接枝丙烯酸(AA)、甲基丙烯酸(MAA)、丙烯酸甲酯(MA)、甲基丙烯酸甲酯(MMA)、丙烯酰胺(AM)等单体,以赋予薄膜表面新的化学性质.考察了引发剂浓度、紫外光的辐照时间、辐照强度、单体种类对LDPE薄膜接枝程度的影响.结果表明,在一定范围内,增加芴酮浓度,可以提高单体的接枝率,但当芴酮浓度达到5%时,接枝率反而下降.延长辐照时间至4 min和提高紫外光的辐照强度达100 W/m2,均有利于接枝反应的进行.不同单体在LDPE膜上的接枝能力与单体的活性、单体与基材的相容性等因素有关.接枝后,LDPE与水的接触角下降程度不仅与单体在膜上的接枝量有关,还与接枝单体的亲水性能密切相关.