离子源辅助电子枪蒸发制备Ge1－xCx薄膜

应用电子枪蒸发纯Ge,考夫曼离子源辅助的方法在Ge基底上沉积了Ge1－xCx薄膜.制备过程中,Ge作为蒸发材料,CH4作为反应气体.通过改变CH4/(CH4+Ar)的气体流量比（G）,制备了G从40％到85％的Ge1－xCx薄膜.应用X射线衍射仪（XRD）测量了Ge1－xCx薄膜的晶体结构,使用傅里叶红外光谱仪（FTIR）测量了2～22 μm的光学透过率,X射线光电子能谱测试（XPS）计算得到C的含量随G的变化关系,用纳米压痕硬度测试计测量了Ge1－xCx薄膜的硬度,原子力显微镜（AFM）测量了G为60％,85％时Ge1－xCx薄膜的表面粗糙度.测试结果表明：制备的Ge1－xCx薄膜在不同的G值下均为无定形结构.折射率随着G值的增加而减小,在3.14～3.89之间可变,并具有良好的均匀性以及极高的硬度.     

GeV能量的Fe离子在C60薄膜中的辐照效应研究

利用傅立叶转换红外光谱和Raman谱仪分析了0.98 GeV的Fe离子在电子能损Se为3.5 keV/nm时， 不同辐照剂量（5×1010 —8×1013 ions/cm2)下， 在C60薄膜中引起的辐照损伤效应。 分析表明， Fe离子辐照引起了C60分子的聚合与损伤。 在辐照剂量达到一中间值1×1012 ions/cm2， C60分子的损伤得到部分恢复， 归因于电子激发引起的退火效应。 通过对Raman数据的拟合分析， 演绎出Fe离子辐照在C60材料中形成的潜径迹截面或引起损伤的截面约为1.32×10-14 cm2。     

Pr3+离子在氟化物玻璃中的光跃迁的计算与分析

测量了Pr(0.5):ZBLAN非晶的吸收光谱,由此利用Judd-Ofelt理论计算了Pr3 离子在材料中的光谱跃迁强度参量,讨论Judd-Ofelt理论在计算Pr3 离子的强度参数时存在的问题.从所得到的强度参数计算预言了此材料中Pr3 离子的各能级之间的自发辐射跃迁速率、荧光分支比和积分发射截面,由所得结果讨论了该材料作为激光材料的前景及可能存在的光子雪崩上转换机制.     

K+和Al3+掺杂对掺Er3+溶胶凝胶玻璃发光特性的影响

通过Sol-gel(溶胶-凝胶)技术,首次将Al3 离子和K 离子同时引入到掺Er3 硅酸盐玻璃中,并测定了硅基玻璃中Er3 离子的吸收光谱、透射光谱、光致发光光谱(PL谱)、上转换光谱、拉曼光谱及荧光寿命.结果显示:掺入的Al3 离子和K 离子不但分别使Er3 离子的荧光强度增强20倍和70倍,而且使Er3 离子在1 532 nm处的荧光寿命从4.8 ms延长至7.1和11.2 ms,但经过进一步分析可知两者对其的影响机制却完全不同;同时作者发现,在980 nm波长激发下,Er3 离子的上转换荧光应该同时存在两种发光机制:双光子吸收和能量传递上转换.     

GaN半导体中InN量子点的结构性质

采用第一性原理模拟计算纤锌矿结构GaN半导体中InN量子点的结构性质。建立64和128个原子的超原胞量子点模型,进行结构优化以获得稳定的吻合实际的系统,并模拟分析电子结构。从态密度空间分布图看到不同轴向的量子势阱形状各异、深度不一,说明量子点的限域效应存在着各向异性的特点。c轴极化方向引起量子点结构带边的弯曲形状与传统的量子阱结构不同,使得电子空穴没有发生空间分离,有利于电子空穴的跃迁几率的提高。     

共掺杂效应对Y2O3:Eu3+和Gd2O3:Eu3+发光影响的理论研究

通过在Y2O3:Eu3 和Gd2O3:Eu3 发光材料中掺入Li ,Mg2 ,Al3 等离子能有效地提高材料的发光强度,根据分子动力学和密度泛函计算的结果,认为这些离子多倾向于形成C2格位附近的间隙缺陷对,导致部分Y(Gd)-O的键长增加,提高了材料的量子效率的同时使得激发峰位出现红移,是引起材料发光增强的一个原因.     

Resonant Response of Rectangular/kFM Cantilever in Liquid

Dynamic characteristics of atomic force microscopy （AFM） cantilevers can be influenced by their working media. We perform an experimental study on the resonant responses of rectangular AFM cantilevers with different sizes immersed in various viscous fluids. The measured resonance frequencies in liquids are used to valldate several theoretical models. Comparison shows the analytical model proposed by Sader [J. Appl. Phys. 84 （1998） 64] can give the best agreement with the experimental results with the maximum relative error nearly 16% for all the cantilevers in different liquids. The ratio between the resonant frequencies in air and water is almost independent of the cantilever length, which is consistent with the theoretical analyses.     

Efficiency Enhancement of Dye-Sensitized Solar Cells： Using Salt CuI as an Additive in an Ionic Liquid

Energy conversion efficiency of the dye-sensitized solar cell is improved from 3.5% to 4.5% by adding a small amount of CuI into an ionic liquid electrolyte. It is found that other copper-I salts, for example, CuBr, have the same effect for the dye-sensitized solar cell. Experimental results show that no Cu^2＋ ions exist in this electrolyte. It is suggested that this improvement is caused by the adsorption of Cu^＋ onto the TiO2 porous film.     

Formation of Pd-Ni Based Bulk Metallic Glasses

Bulk metallic glasses are prepared in Pd4o.sNi4o.sSixP19-x （x = 0-14 at.%） alloys by a combination of flux treatment and water quenching technique. It is found that the thermal stability of the Pd4o.sNi4o.sSixP19=x glassy alloys depends on the addition of Si content. Among the Pd4o.sNi4o.sSixP19=x glassy alloys studied, the Pd4o.sNi4o.sSisPls bulk metallic glass exhibits the largest supercooled liquid region （△T = 119 K） and the highest activation energy of crystallization （283.3k J/tool）, showing enhanced glass formation ability and extraordinary glassy thermal stability.     

Multiple ionization of argon accompanied by electron loss and capture of 0.22-6.35 MeV C^q＋ ions

In this paper a projectile ions recoil ions coincidence technique is employed to investigate the target ionization and projectile charge state changing processes in the collision of 0.22-6.35 MeV Cq^＋ （q = 1 - 4） ions with argon atoms. The partial cross section ratios of the double, triple, quadruplicate ionization to the single ionization （or the single capture） of argon associated with single electron loss （or single electron capture） by the projectile are measured and compared with the previous experimental results. In the present experiment, it is observed that the ratios of ionization cross sections R associated with single loss and single capture depend strongly on the projectile charge state and vary significantly with different reaction channels as impact energy increases. In addition, this paper gets empirical scaling laws for the ionization cross section ratios R corresponding to the projectile single loss and finds that the ratios of the double ionization to the single ionization associated with single electron capture remain constant in the present energy range.