CiADS束流负载效应前馈补偿的仿真评估

在高功率超导质子直线加速器中，束流负载效应是影响超导腔幅相稳定性的一个重要因素。本工作基于谐振腔建场模型，开发了超导腔系统束流负载效应的时域仿真程序，分析了束流负载效应对超导腔幅相稳定性的影响，并在C-ADS注入器II上通过相关实验测量对仿真结果进行了验证。利用该程序，评估了CiADS超导直线加速器脉冲束流的脉冲长度，以及前馈补偿的时序抖动和束流纹波等因素对腔中电磁场幅相稳定度的影响。仿真结果表明:在当前CiADS直线加速器设计参数下，为满足超导腔中电磁场0.1%与在高功率超导质子直线加速器中，束流负载效应是影响超导腔幅相稳定性的一个重要因素。本工作基于谐振腔建场模型，开发了超导腔系统束流负载效应的时域仿真程序，分析了束流负载效应对超导腔幅相稳定性的影响，并在C-ADS注入器II上通过相关实验测量对仿真结果进行了验证。利用该程序，评估了CiADS超导直线加速器脉冲束流的脉冲长度，以及前馈补偿的时序抖动和束流纹波等因素对腔中电磁场幅相稳定度的影响。仿真结果表明:在当前CiADS直线加速器设计参数下，为满足超导腔中电磁场0.1%与$0.1^{\circ}$的幅相稳定度指标，前馈时序抖动的偏差不能超过0.79 μs，束流流强的直流偏差不能超过0.9%，并且给出了束流纹波的最大抖动幅值与纹波频率之间的关系。这些结果将为CiADS超导直线加速器相关子系统技术指标的确定提供依据。     

Ca9Al(PO4)7∶Eu2+的发光、浓度猝灭及温度稳定性

采用高温固相法制备了Ca9Al(PO4)7∶Eu2+蓝色荧光粉,研究了Ca9Al(PO4)7∶Eu2+的发光、浓度猝灭及温度稳定性.Ca9Al(PO4)7∶Eu2+的激发光谱覆盖200～350 nm紫外区;发射光谱为一主峰位于445 nm的宽谱,对应Eu2+的4f6 5d1--→4f特征跃迁.研究发现,随Eu2+掺杂量的增大,Ca9Al(PO4)7∶Eu2+的发射强度呈现先增大、后减小的变化趋势,最大发射强度对应的Eu2+掺杂量为0.01,即存在浓度猝灭效应,对应的机理为电偶极-电偶极相互作用;依据晶格常数,得出临界距离为2.297 nm.在25～300℃范围内改变光谱测量温度,发现温度升高到150℃时,Ca9Al(PO4)7∶Eu2+的发射强度变为25℃时的81.0％,对应的激活能为0.268 eV,说明材料具有较好的温度稳定性.     

Can secondary nucleation exist in ice banding of freezing colloidal suspensions?

The formation mechanism of ice banding in the system of freezing colloidal suspensions, which is of significance in frost heaving, ice-templating porous materials and biological materials, is still a mystery. Recently, the theory of secondary nucleation and growth of ice has been proposed to explain the emergence of a new ice lens. However, this theory has not been quantitatively examined. Here, we quantitatively measure the initial interfacial undercooling of a new ice lens and the nucleation undercoolings of suspensions. We find that the interfacial undercooling cannot satisfy the nucleation undercooling of ice and hence disprove the secondary nucleation mechanism for ice banding.     

The effect of interfacial energy anisotropy on planar interface instability in a succinonitrile alloy under a small temperature gradient

The morphological stability of a planar interface with different crystallographic orientations is studied under a small positive temperature gradient using a transparent model alloy of succinonitrile.Novel experimental apparatus is constructed to provide a temperature gradient of about 0.37 K/mm.Under this small temperature gradient,the planar interface instability depends largely on the crystallographic orientation.It is shown experimentally that the effect of interfacial energy anisotropy on planar interface stability cannot be neglected even in a small temperature gradient system.Higher interfacial energy anisotropy leads the planar interface to become more unstable,which is different from the stabilizing effect of the interfacial energy on the planar interface.The experimental results are in agreement with previous theoretical calculations and phase field simulations.     

氢原子谱线与高质量金刚石薄膜

采用蒙特卡罗方法,对以CH₄/H₂混合气体为源气体的电子助进热丝化学气相沉积(EACVD)中的氢原子发射过程进行了模拟。在模拟中考虑了电子与H₂的弹性碰撞及振动激发、分解、电子激发(包括H_α, H_β, H_γ谱线的激发)、电离及分解电离等非弹性碰撞过程;与CH₄的碰撞考虑了弹性动量传输及振动激发、分解、电子激发、分解激发(包括H_α, H_β, H_γ谱线的激发)、电离及分解电离等非弹性碰撞过程。研究了不同实验条件下产生的H, CH₃的数目与氢原子谱线相对强度的关系,给出了一种利用氢原子谱线来获得最佳成膜实验条件的方法。对于有效控制工艺条件,生长出高质量的金刚石薄膜具有重要意义。     

Ultraviolet emission of ZnO film prepared by electrophoretic deposition

We deposited high quality ZnO film by electrophoretic deposition (EPD) using high quality ZnO powder prepared by solid-state pyrolytic reaction. X-ray photoelectron spectroscopy (XPS) and the infrared (IR) absorption spectrum clearly indicate that the ZnO phase powder has been prepared. Transmission electron microscope (TEM) imaging and x-ray diffraction (XRD) show that the average grain size of the powder is about 20nm. XRD and selected-area electron diffraction (SAED) reveal that the ZnO film has a polycrystalline hexagonal wurtzite structure. Only a strong ultraviolet emission peak at 390nm can be observed at room temperature.     

求解stokes问题的一个新的非协调混合元格式

构造一个新的非协调混合元格式求解stokes问题,证明了该元满足B-B条件,并且有2阶收敛速度.     

基于异构三联苯-2，2″，4，4″-四羧酸构筑的单水桥钴(Ⅱ)、镍(Ⅱ)配位聚合物的合成、结构及磁性质

使用异构三联苯-2,2″,4,4″-四羧酸配体(m-H₄tpta和p-H₄tpta),通过水热法合成了2例新的单水桥Co (Ⅱ)/Ni (Ⅱ)金属链状配位聚合物[Co (m-H₂tpta)(H₂O)₃]_n(1)和{[Ni₂(p-tpta)(H₂O)₆]·2H₂O}_n(2)。其结构通过FT-IR、元素分析、X射线单晶及粉末衍射进行了表征。在结构上,金属离子呈现出轻微扭曲的八面体几何构型,通过单水分子桥连接形成了一维金属链,异构H₄tpta配体分别采用μ₁-η¹∶η⁰∶η¹∶η⁰和μ₄-η¹∶η¹∶η¹∶η¹配位模式与金属离子连接,形成一维链和三维网状结构,配合物2表现出(4,4)-连接的NbO型的三维拓扑网络结构。磁性方面,配合物1的Co(Ⅱ)离子间通过μ₂-H₂O桥传递表现出反铁磁相互作用。配合物2也展现出Ni(Ⅱ)离子间的反铁磁耦合作用,与磁耦合Ni—Ow—Ni角有关。     

Full period superconducting section physics design for injector Ⅱ of China-ADS

The China Accelerator Driven Subcritical System (China-ADS) project, which is a strategic plan and aims to design and build an ADS demonstration facility, has been proposed and launched actively in China. Injector Ⅱ as one of the parallel injectors of China-ADS, and is prompted by the Institute of Modern Physics (IMP). In this paper, a new scheme with full period lattice structure for the SC section is proposed. In the new scheme, there are sixteen periods, with one superconducting solenoid and one superconducting cavity included in each period. All of the elements are contained in four cryomodules. The dreadful influence of the mismatch caused by period structural change can be avoided, and the beam quality is favorable. In addition, this new scheme has certain advantages in reducing the project's difficulty and construction risk. The details of the design and beam dynamic simulation for the full period lattice structure are given in this paper.     

基于嵌入式系统的射频超导量子干涉仪控制系统

本文介绍了嵌入式系统在射频超导量子干涉仪控制系统中的应用,提出了嵌入式系统的整体方案,并对系统工作原理以及设计思想做了简要介绍.