超导金属玻璃Zr78Co22的结晶化动力学研究

综合利用x射线小角散射、广角衍射、场离子显微镜等测量,并结合超导临界温度和显微硬度的观测,研究了金属玻璃Zr₇₈Co₂₂的结构及其结构弛豫和结晶化过程.结果表明,淬态金属玻璃Zr₇₈Co₂₂中存在明显的相分离,其中一个相的组分似乎趋向于纯Zr,另一相的组分则与ZO₄Co接近.在结构弛豫过程中,主要是拓扑短程序发生了变化,它受成核长大机理支配.当核的数量足够多时,两相均匀一致地长大. 关键词：     

光学微操纵过程的轴平面显微成像技术

光学俘获技术利用光与物质相互作用产生的光势阱效应来实现对微粒的操控,已经成功应用于生物医学、材料科学等交叉领域.在对微粒进行三维俘获时,传统的宽场光学显微技术只能观测到某一平面内微粒的横向运动,对微粒沿轴向运动的观测受到很大限制.本文将轴平面显微成像技术引入光学微粒操控研究中,利用45?倾斜的反射镜把微粒的轴向运动信息转换到横向平面进行观测,与传统宽场显微成像技术相结合,实现了对二氧化硅小球俘获过程横向和轴向运动的同步观测.该成像方法无需扫描和数据重构,具有实时快速等优点,在新型光束光镊、厚样品三维观测和成像等领域具有潜在的应用价值.     

Y+SO2反应动力学成像

本文利用时间切片离子速度成像技术、交叉分子束和激光溅射技术研究了高碰撞能下(36 kcal/mol)钇原子与二氧化硫分子的反应动力学. 利用多光子电离在482∽615 nm的波长范围内得到了产物YO的时间切片离子速度成像. YO的切片图像显示其较宽的速度分布和前-后向散射为主的角分布,其中前向散射信号明显强于后向散射. 这种空间分布暗示了该反应通过一个中间体进行,且中间体的寿命不超过一个转动周期. 中间体的形成意味着该氧化反应电子转移机理的发生.     

碱金属阳离子对[B3O7]型非线性光学晶体结晶习性的影响

本文利用高温拉曼光谱技术和从头计算的方法, 研究了LiB₃O₅和CsB₃O₅晶体高温熔融体的结构, 分析了碱金属阳离子对熔体结构的影响, 以及熔体结构的差异与LiB₃O₅和CsB₃O₅晶体结晶习性的联系. 结果表明: LiB₃O₅和CsB₃O₅晶体高温熔融体中的结构基团 主要为B₃Ø₇和B₃Ø₆两种不同类型的硼氧六元环; 环内BØ₄ 四面体的数量影响了六元环呼吸振动峰的拉曼频率, 随BØ₄四面体数量的增加六元环呼吸振动峰向低频移动; LiB₃O₅晶体高温熔融体中, BØ₄四面体含量相对较多; 然而, 离子半径相对较大的Cs⁺离子却阻碍了熔体中BØ₄四面体的形成, 造成CsB₃O₅晶体高温熔融体中BØ₄/BØ₃比值的降低. 结合LiB₃O₅和CsB₃O₅晶体生长动力学过程的分析 (Wang D, Wan S M et al. 2011 Cryst. Eng. Comm. 13 5239), 阳离子的不同导致高温熔体中BØ₄四面体数量的差异, 被认为是影响LiB₃O₅和CsB₃O₅晶体结晶习性的重要因素, 有效降低高温熔体中BØ₄四面体的数量, 将是实现LiB₃O₅晶体生长的关键条件. 关键词： 硼酸盐晶体 熔体结构 拉曼光谱 结晶习性     

飞秒时间分辨离子成像研究NO2分子通道分辨超快解离动力学

本文利用飞秒激光泵浦-探测质谱和离子成像研究了NO_2分子的超快解离动力学.结果表明NO~+离子的动能释放包含两个部分,分别对应的能量是0.05和0.25 eV,并且指认了它们叫能的解离通道.NO~+离子通道分辨的瞬态测量提供了区分超快解离路径贡献的方法,不同动能释放的离子信号变化曲线可以通过双e指数函数进行拟合.其中衰减时间为0.25 ps的快速变化部分产生于里德堡态的演化.变化较慢的信号部分是山两个竞争的通道产生的,其中一个通道是吸收一个400 nm光子到A~2B_2激发态,它的衰减寿命是30 ps;另一个慢的通道是吸收三个400 nm光子到一个价电子类型的里德堡态,它的衰减寿命是短于7.2 ps.通道和时间分辨的实验测量对于区分分子复杂的超快解离动力学具有非常大的潜力.     

结合虚拟单像素成像解卷积的双边照明光片荧光显微技术

光片荧光显微术(light-sheet fluorescence microscopy,LSFM)采用薄片光束从侧面激发样品,在垂直于光片方向上进行成像,具有成像速度快、光学层析能力强以及光漂白和光毒性低等优点,适用于对较大活体生物样品进行高质量、长时间三维动态观测.然而,传统高斯光束LSFM存在分辨率低和成像视场小的...     

激光限制结晶技术制备nc-Si/SiO2多层膜

在等离子体增强化学气相淀积系统中，采用aSi:H层淀积和原位等离子体氧化相结合的逐层生长技术制备了aSi:H/SiO_2多层膜.在激光诱导限制结晶原理基础上，使用KrF准分子脉冲激光为辐照源，对aSi:H/SiO_2多层膜进行辐照，使纳米级厚度的aSi:H子层晶化.Raman散射谱和电子衍射谱的结果表明，经过激光辐照后纳米Si颗粒在原始的aSi:H子层内形成，晶粒尺寸可以根据aSi:H层的厚度精确控制.还研究了样品的光致发光（PL）特性以及激光辐照能量密度对PL性质的影响. 关键词： 脉冲激光 多层膜 限制结晶     

纳米颗粒近场空间光谱散射建模与显微成像分析

用非直观偏振参数显微成像,即采用在传统显微光路中插入模式化装置,通过拟合过滤后对所得数据反演成像,通过对金属纳米颗粒在近场空间散射光谱分析,来解决空间散射现象。用非直观偏振参数显微成像与传统直观成像做对比,并通过时域有限差分法建模仿真,来描述近场直观与非直观散射光谱的差异,对比结果发现,非直观偏振参数显微反演成像的分辨率比直观成像更高,不但能够清晰的探测到纳米颗粒的形状和电场分布,而且比直观成像获得更广泛的空间散射光谱。     

在193 nm关于Si2分子的离子解离动力学的成像研究

在193 nm的单色激光实验中,本文利用时间切片离子速度成像技术,研究了经193 nm双光子电离得到的Si₂⁺的解离反应动力学过程. 根据实验得到的Si⁺离子的速度成像,观测到了两种离子直接解离通道：Si(³P_g)+Si⁺(²P_u)和Si(¹D₂)+Si⁺(²P_u). 电子基态的Si₂分子处于v=0∽5的振动态上,其经过双光子电离后激发到Si₂⁺离子的多个电子激发态势能面,生成主要通道Si(³P_g)+Si⁺(²P_u),其中v=1的解离信号最强. 此外,由于势能曲线2²Π_g与3²Π_g相同对称性引起的避免性势能面交叉,生成次要反应通道Si(¹D₂)+Si⁺(²P_u). 通道Si(¹D₂)+Si⁺(²P_u)的产物亦可以由生成的基态Si₂⁺(X⁴Σ_g^-)吸收一个193 nm光子后解离得到,其对应产物则具有更大的动能.     

样品表面银膜的粗糙度对钛酸钡微球成像性能的影响

研究了样品表面镀有不同表面粗糙度的银膜对钛酸钡（BaTiO₃ glass,BTG）微球成像效果的影响,发现当银膜表面的粗糙度（RMS）从3.23 nm增大到6.80 nm时,用直径为15 μm的BTG微球观察直径为250和580 nm的微球阵列,样品的成像范围增大.另外,BTG微球还可以清晰分辨原本不可分辨的直径为200 nm的微球阵列.结果表明,粗糙银膜引起的散射作用和表面等离激元波的局域场增强效应,使得更多物体的高频信息耦合进微球,提高了微球成像的分辨率和成像范围.     

Optical conductivity of CePd3, YPd3 and PrPd3

The optical conductivity of intermediate valence CePd₃ at 300 K exhibits a maximum near 16 meV, which is absent in the reference materials YPd₃ and PrPd₃. Using a modified Drude model with a memory function ansatz this anomaly has been identified as a resonant electron-electron scattering process of conduction electrons at the localized 4f states near the Fermi level E_F. The model fit gives estimates of the width of the 4f states, of their separation from E_F and of the f-d hybridization energy. Intra-4f transitions of CePd₃ are stronger compared to those of PrPd₃ due to the stronger f-d hybirdization. 4d→4f transition energies of CePd₃ are reduced due to an electron-hole Coulomb binding energy.     

Observation of ZnO nanoparticles outside pores of nano Zn4O(C8H4O4)3 metal-organic framework

It was recognized that ZnO can be formed during synthesizing nano Zn₄O(C₈H₄O₄)₃ metal-organic framework (nano MOF-5). Furthermore, it is generally accepted that the ZnO is dispersed inside the pores of MOF-5. However, herein, the measurements of X-ray powder diffraction (XRD) and transmission electron microscopy (TEM) showed that the crystal particle sizes of ZnO in MOF-5 are in the range of 5-18 nm, which are larger than the pore size of MOF-5 (1.3 nm). This clearly demonstrates that those ZnO nanoparticles are located outside the pores of MOF-5.     

Al2O3对氟氧化物玻璃微结构和析晶的影响

采用红外, Raman, X射线衍射测试分析方法, 研究了Al₂O₃对氟氧化物玻璃微结构和析晶的影响.结果表明, Al³⁺主要以[AlO₄]的形式与[SiO₄]以顶角相连的方式构成基本网络骨架, Al₂O₃含量的增加, 使氧化物玻璃基质的网络向单体和二聚体结构转变, 并使氟化物微晶尺寸有一个先变小后增大的趋势, 但不影响微晶结构.     

Properties of rubidium nitrate in ion-conducting RbNO3-Al2O3 nanocomposites

Properties of RbNO₃ in (1 − x)RbNO₃-xAl₂O₃ nanocomposites were studied by X-ray powder diffraction, electron diffraction, conductivity measurements, infrared and Raman spectroscopy, and differential scanning calorimetry. All the experimental techniques used indicate the presence of an amorphous RbNO₃ layer at the RbNO₃---Al₂O₃ interface in addition to a crystalline RbNO₃ phase. Its concentration was determined from the phase transition enthalpies. The amorphous layer thickness estimated by means of a simple brick-wall model is 4 nm.     

Preparation and characterization of slice-like Cu2(OH)3NO3 superhydrophobic structure on copper foil

Superhydrophobic structure was prepared on copper foil via a facile solution-immersion method. Thus slice-like Cu₂(OH)₃NO₃ crystal was prepared on the surface of the copper foil by sequential immersing in an aqueous solution of sodium hydroxide and cupric nitrate. And the superhydrophobic structure was obtained by modifying the slice-like Cu₂(OH)₃NO₃ crystal with 1H,1H,2H,2H-perfluorodecyltriethoxysilane (FAS-17). The morphologies, chemical compositions and states, and hydrophobicity of the surface-modifying films on the copper foil substrates were analyzed by means of scanning electron microscopy (SEM), X-ray photoelectron spectroscopy (XPS), and water contact angle measurement. Moreover, the thermal stability of the slice-like structure was also evaluated using thermogravimetric analysis (TGA). It was found that roughening of the copper foil surface helped to increase the hydrophobicity to some extent, but no superhydrophobicity was obtained unless the slice-like Cu₂(OH)₃NO₃ crystal formed on the Cu substrate was modified with 1H,1H,2H,2H-perfluorodecyltriethoxysilane. Besides, the superhydrophobicity of the FAS-17-modified slice-like Cu₂(OH)₃NO₃ structure was closely related to the surface morphology. And this hydrophobic structure retained good superhydrophobic stability at elevated temperature and in long-term storage as well, which should be critical to the application of Cu-matrix materials in engineering.     

Optical properties and electronic structure of CsPbCl3 and CsPbBr3

Optical measurements of CsPbCl₃ and CsPbBr₃ layers and crystals are reported. They are explained with an empirical LCAO-scheme which shows the close relationship to the polymorphous thallous halides.     

SrHfO3和SrTiO3光学特性的第一性原理研究

用全电势线性缀加平面波法(FLAPW)计算了SrTiO₃和SrHfO₃的光学特性，即介电函数虚部ε₂(ω)、光学吸收系数I(ω)和反射率R(ω).对它们光学特性进行了对比分析，给出了它们光学特性的差别，并进行了解释.计算的SrTiO₃光学谱分别在4.4，7.4，8.3和23.6eV处出现峰值，且其在4.4eV处的峰值比较高而尖.计算结果与实验值符合得很好. 关键词： 平面波法计算 光学常量和参数 铁电体     

Optical band-gap of Zn3As2

Absorption measurements of single Zn₃As₂ crystals were made at temperatures 5, 80 and 300 K. Free-carrier absorption is interpreted in the simple classical model. Interband absorption shows contributions from Urbach-like excitations. The direct optical gap has been estimated as 0.99 eV at 300 K, 1.09 eV at 80 K and 1.11 eV at 5 K. The linear dependence of band-gap on temperature was found in the range 80–300 K with dE_g/dT = ? 4.55 × 10^?4eVK^?1.     

Optical properties of Tl3SbS3 acousto-optic crystals

Optical properties of acousto-optical material Tl₃SbS₃ were investigated at the fundamental absorption edge. The basic (n = 1) and excited (n = 2, 3) exciton states were obtained from the λ-modulated reflection spectra for polarizations E⊥c at 10 K. Taking into account the spatial dispersion we determined the parameters of excitons by calculating the spectra shapes of λ-modulated reflection of line n = 1 and estimated values of the zone-translation masse and the reduced effective masse of excitons, the effective masse of electrons , heavy and light holes.