ICF模拟靶和低温冷冻气体的表征

由于DT或DD固态层的折射率很低，而且，其厚度只有几微米到几十微米。这使得光通过DT或DD燃料层时产生的光学路径也只有几微米到几十微米，远小于ICF靶丸。因此，尽管长期以来使用传统的光学干涉仪测定透明ICF靶丸的壁厚，它们却很难用来精确测定DT或DD固态层的厚度。相反，全息照相技术允许直接测定燃料层的厚度，而极大地忽略ICF靶丸的壁厚。在现在的研究中，已经建立全息照相装置，并且已用来测量ICF模拟靶丸的壁厚和气体的厚度。     

Nitrogen Adatom Diffusion on a Ga－Rich GaN （0001） Surface

The diffusion of N adatoms on a Ga-rich GaN(O001) surface has been studied using density-functional theory.The configuration of Ga adatoms on a Ga-rich GaN surface has been identified. The first adlayer Ga adatoms are on top of the terminating substrate Ga atoms, and the outmost adlayer Ga adatoms exist randomly at the T4 or H3 sites. A very different diffusivity of N adatoms on a Ga-rich GaN(0001) surface has been found. The excess Ga adatoms on a GaN(0001) surface reduce the diffusion barrier by 0.75eV and influence the migration path. It seems that bilayer Ga adatoms are helpful for N atom diffusion.     

霍尔推进器的研究现状与发展趋势

电推进是利用电能加热、离解和加速工质，使其形成高速射流而产生推力的技术。与化学推进相比，电推进具有比冲高、推力小、能重复启动、重量轻和寿命长等特点，因而电推进可用作航天器的姿态控制、轨道转移和提升、轨道修正、阻力补偿、位置保持、重新定位、离轨处理、宇宙探测和星际航行等任务。     

Evolving Networks with Nonlinear Assignment of Weight

We propose a weighted evolving network model in which the underlying topological structure is still driven by the degree according to the preferential attachment rule while the weight assigned to the newly established edges is dependent on the degree in a nonlinear form. By varying the parameter a that controls the function determining the assignment of weight, a wide variety of power-law behaviours of the total weight distributions as well as the diversity of the weight distributions of edges are displayed. Variation of correlation and heterogeneity in the network is illustrated as well.     

ICF靶用泡沫铜的制备与表征

 以次磷酸钠为还原剂的化学镀进行导电化处理,研究了ICF靶用泡沫铜的电沉积工艺。采用扫描电子显微境和X射线衍射仪对制备过程中各阶段泡沫铜的微观结构进行了表征。结果表明：经化学镀后可获得晶粒尺寸小、分布均匀的铜沉积层。电沉积后铜沉积层主要由0.55 μm的小颗粒组成,并且出现突出大颗粒的形貌特征。在氢气氛围下,经700 ℃热处理后,铜颗粒进一步长大,沉积层结晶致密。制备的泡沫铜呈3维网络状结构,分布均匀,密度为0.19 g/cm³,孔径分布为400～600 μm,孔隙率达97.9％。     

ICF靶用微球弹跳的影响因素分析

 通过对微球弹跳模型的建立,对微球弹跳过程进行了受力分析,解释了微球弹跳过程中遇到的微球粘连或“不跳”、弹跳率起伏不定及弹跳幅度高低不同等现象。通过对加载信号方向与大小、微球质量及尺寸大小、微球及反弹盘表面特性、环境湿度等影响微球弹跳效果因素的分析,提出了改善涂层表面粗糙度和弹跳效果的措施,包括根据微球大小调整微球弹跳激励方式、等离子体中和微球表面电荷、反弹盘表面改性减小球盘之间的相互作用力。     

Optical Properties of Co-BaTiO3/Mg（100） Nano-Composite Films Grown by Pulsed Laser Deposition Method

Co nanoparticles embedded in a BaTiO3 matrix, namely Co-BaTiO3 nano-composite films are grown on Mg（100） single crystal substrates by the pulsed laser deposition （PLD） method at 650℃. Optical properties of the CoBaTiO3 nano-composite films are examined by absorption spectra （AS） and photoluminescence （PL） spectra. The results indicate that the concentration of Co nano-particles strongly influences the electron transition of the Co BaTiO3 nano-composite films. The PL emission band ranging from 1.9 to 2.2eV is reported. The AS and PL spectra suggest that the band gap is in the range of 3.28-3.7eV.     

Self-Injection and Acceleration of Monoenergetic Electron Beams from Laser Wakefield Accelerators in a Highly Relativistic Regime

Self-injection and acceleration of monoenergetic electron beams from laser wakefield accelerators are first investigated in the highly relativistic regime, using 100 TW class, 27 fs laser pulses. Quasi-monoenergetic multi- bunched beams with energies as high as multi-hundredMeV are observed with simultaneous measurements of side-scattering emissions that indicate the formation of self-channelfing and self-injection of electrons into a plasma wake, referred to as a ＇bubble＇. The three-dimensional particle-in-cell simulations confirmed multiple self-injection of electron bunches into the bubble and their beam acceleration with gradient of 1.5 GeV/cm.     

基于多维混合柯西分布的点云配准

为提高三维点云在数据随机缺失和噪声干扰等复杂情况下的配准精度,提出一种基于多维混合柯西分布(MMC)的点云配准方法。将点云数学模型扩展为MMC模型,求解模型各参数,并构造出特征四面体,以优化旋转矩阵与平移向量;通过最大期望算法分别求出目标点云和待配准点云在MMC模型下的数据中心、协方差矩阵和权重的值。仿真与实验数据表明:与几种常用的算法相比,MMC算法即使在点云数据存在遮挡、缺失,大小不一致,含随机噪声,且具有无序性的条件下,也能精确配准,且具有良好的稳健性。     

水流损失和热补偿共同作用对增强型地热系统(EGS)产能影响的研究

基于青海共和盆地-3705m地热田实测数据,结合流固耦合传热理论并运用Comsol软件,建立了离散型裂隙岩体流体传热模型。考虑水流损失和热补偿共同作用,模拟得到了开采过程中上、下岩层(盖层和垫层)为绝热不渗透、传热不渗透、渗透传热时,储层(上、下岩层和压裂层)温度场的变化特征,分析了产出流量、水流损失、产出温度、产热速率的变化规律。研究结果表明:采热过程中产出流量始终小于注入流量;产出流量增幅速率先增大后减小,最后趋于稳定,前3a产出流量增幅超过总增幅量的3/4;忽略水流损失,将高估产热速率,采热初期甚至达到考虑水流损失时产热速率的3倍以上;考虑水流损失,产热速率呈先快速上升再趋于稳定后逐渐下降的趋势,最优开采时间为3a^11a;研究上、下岩层对产出温度的影响,仅考虑传热,采热寿命延长5.43%,同时考虑渗流传热时,采热寿命延长2.71%;采热前9a,水流损失占主导作用,即流入上、下岩层水流损失对产热速率的影响高于热补偿效应,开采10a后,热补偿效应占主导作用;同时考虑水流损失和热补偿效应得到的产热速率变化规律与实际工程更为符合,建议选择低渗透能力的上、下岩层延长增强型地热系统(EGS)运行时间。