电子电气产品中挥发性有机化合物的释放量测定

采用小型释放舱-热脱附-气相色谱-质谱联用技术测定了电子电气产品中8种挥发性有机化合物（苯、甲苯、邻二甲苯、间二甲苯、对二甲苯、乙苯、乙酸丁酯和苯乙烯）的释放量.对一级脱附参数（一级脱附温度、一级脱附流量、一级脱附时间）、冷阱温度、捕集管脱附温度、脱附时间条件进行了优化,并进行了线性关系、回收率、精密度等试验.结果表明：本方法可用于测定电子电气产品中释放的8种常见的挥发性有机化合物的释放量,线性范围10-1000ng,当采样量为6L时,定量限为1.7μg/m3,回收率范围在89.5％-106％之间,相对标准偏差小于7％.     

大口径激光玻璃环抛光学沥青抛光胶

研制了四种不同沥青和松香含量的光学沥青抛光胶,对其形貌、针入度、玻璃化转变温度、软化点和粘度等参量进行了表征。从组成和结构分析了抛光胶三种物理状态变化原因,将玻璃化转变温度和软化点作为其临界转变温度。实验研究了四种抛光胶对大口径激光玻璃的抛光效果,发现抛光胶中沥青和松香的质量分数分别为30%和70%时,抛光效果比较理想,在像散和表面疵病控制方面能够满足要求,可作为大口径激光玻璃抛光专用胶。     

Conception design of helium ion FFAG accelerator with induction accelerating cavity

Technological advancements are strongly required to fulfill the demands of new accelerator devices with the highest accelerating gradients and operation reliability for the future colliders.To this purpose an extensive R&D regarding molybdenum coatings on copper is in progress.In this contribution we describe chemical composition,deposition quality and resistivity properties of diferent molybdenum coatings obtained via sputtering.The deposited films are thick metallic disorder layers with diferent resistivity values above and below the molibdenum dioxide reference value.Chemical and electrical properties of these sputtered coatings have been characterized by Rutherford backscattering,XANES and photoemission spectroscopy.We will also consider multiple cells standing wave section coated by a molybdenum layer designed to improve the performance of X-Band accelerating systems.     

熔石英亚表面缺陷附近光强分布的数值模拟

 熔石英亚表面缺陷对光场的调制是导致激光辐照场破坏的主要因素。采用有限元方法对熔石英亚表面缺陷（平面和锥形划痕）周围的光强分布进行了数值模拟。结果表明：划痕形状、几何尺寸、方位角、光的入射角等是影响划痕周围光强分布的主要因素;前表面划痕对光强的增强效果比后表面弱;在理想形状的划痕截面和表面同时发生内全反射时,平面划痕周围的光强增强效果明显。锥形划痕周围的光强分布为正确解释交叉划痕的夹角平分线附近的损伤提供了理论依据。     

Resonant Tunnelling and Storage of Electrons in Si Nanocrystals within a-SiNx/nc-Si/a-SiNx Structures

The a-SiNx/nanocrystalline silicon （nc-Si）/a-SiNx sandwiched structures with asymmetric double-barrier are fabricated in a plasma enhanced chemical vapour deposition （PECVD） system on p-type Si substrates. The nc-Si layer in thickness 5nm is fabricated from a hydrogen-diluted silane gas by the layer-by-layer deposition technique. The thicknesses of tunnel and control SiNx layers are 3nm and 20nm, respectively. Frequency-dependent capacitance spectroscopy is used to study the electron tunnelling and the storage in the sandwiched structures. Distinct frequency-dependent capacitance peaks due to electrons tunnelling into the nc-Si dots and capacitance-voltage （C - V） hysteresis characteristic due to electrons storage in the nc-Si dots are observed with the same sample. Moreover, conductance peaks have also been observed at the same voltage region by conductance-voltage （G - V） measurements. The experimental results demonstrate that electrons can be loaded onto nc-Si dots via resonant tunnelling and can be stored in our a-SiNx/nc-Si/a-SiNx structures.     

2018年10期 电子期刊

采用自蔓延燃烧法结合高温热处理方法制备了镝离子掺杂浓度不同的七铝酸十二钙（12CaO·7Al₂O₃:x% Dy³⁺,C12A7:x% Dy³⁺） X射线荧光粉材料。实验发现,该系列荧光粉在350 nm激发下,可观察到位于486 nm和575 nm的两个发光峰,其分别来源于Dy³⁺离子的⁴F_9/2→⁶H_15/2和⁴F_9/2→⁶H_13/2跃迁。当镝掺杂摩尔分数为0.3%时,两个发光峰的发射强度最大。在氮气气氛下,1 300℃热处理C12A7:x% Dy³⁺荧光粉后,与未热处理样品相比,笼中OH^-基团减少,导致其光激励发光强度显著增大,并产生了更多的深陷阱。通过使用氮气气氛热处理后的C12A7:0.3% Dy³⁺粉末制成的成像板,以包覆有绝缘层细电线为成像目标,发现在合适的X射线吸收剂量下（0.54 Gy）,可以实现高质量的X射线成像。以上实验结果表明,镝掺杂的七铝酸十二钙X射线荧光粉材料在数字化静态X射线图像目标检测技术中有潜在的应用前景。     

HLS储存环高频调制实验

在合肥光源(HLS)储存环上进行了高频调制实验, 结果表明采用调制频率接近同步振荡频率f_s的高频幅度或相位调制, 可以提高束流寿命. 而通常采用的是2f_s的调制方式. 实验测量了最佳调制频率和合适的调制度, 以及不同流强下调制引起寿命增长的程度. 同时观察到束流频谱中高次分量的降低, 这有利于抑制多束团耦合不稳定性.     

Symmetry and asymmetry rogue waves in two-component coupled nonlinear Schrdinger equations

By means of the modified Darboux transformation we obtain some types of rogue waves in two-coupled nonlinear Schr ¨odinger equations.Our results show that the two components admits the symmetry and asymmetry rogue wave solutions,which arises from the joint action of self-phase,cross-phase modulation,and coherent coupling term.We also obtain the analytical transformation from the initial seed solution to unique rogue waves with the bountiful pair structure.In a special case,the asymmetry rogue wave can own the spatial and temporal symmetry gradually,which is controlled by one parameter.It is worth pointing out that the rogue wave of two components can share the temporal inversion symmetry.     

Investigations of the dielectronic recombination of phosphorus-like tin at CSRm

The electron–ion recombination for phosphorus-like~(112) Sn~(35+)has been measured at the main cooler storage ring of the Heavy Ion Research Facility in Lanzhou, China, employing an electron–ion merged-beams technique. The absolute total recombination rate coefficients for electron–ion collision energies from 0 e V–14 e V are presented. Theoretical calculations of recombination rate coefficients were performed using the Flexible Atomic Code to compare with the experimental results. The contributions of dielectronic recombination and trielectronic recombination on the experimental rate coefficients have been identified with the help of the theoretical calculation. The present results show that the trielectronic recombination has a substantial contribution to the measured electron–ion recombination spectrum of~(112)Sn~(35+). Although a reasonable agreement is found between the experimental and theoretical results the precise calculation of the electron–ion recombination rate coefficients for M-shell ions is still challengeable for the current theory.     

Calculation of the surface energy of fcc metals with modified embedded-atom method

The surface energies for 38 surfaces of fcc metals Cu, Ag, Au, Ni, Pd, Pt, A1, Pb, Rh and Ir have been calculated by using the modified embedded-atom method. The results show that, for Cu, Ag, Ni, A1, Pb and Ir, the average values of the surface energies are very close to the polycrystalline experimental data. For all fcc metals, as predicted, the close-packed (111) surface has the lowest surface energy. The surface energies for the other surfaces increase linearly with increasing angle between the surfaces (hkl) and (111). This can be used to estimate the relative values of the surface energy.