金纳米空心半球壳膜的可调谐光学性质研究

以单层聚苯乙烯微球阵列为模板,通过控制其表面金膜蒸镀时间,制备了具有不同厚度的空心半球壳结构的金纳米膜.利用扫描电子显微镜和自制光谱仪分别测量了金膜表面形貌和其透射光谱,并分析了金膜形貌与其光学性质间的关系,同时以4-巯基苯胺为探针分子测定了金膜的表面增强喇曼散射效应.结果表明,该金纳米膜的表面等离子体共振波长随膜厚度增大而发生红移,在可见与近红外波段较宽范围内可调谐,并且,当金膜共振波长与入射激发光波长较近时,探针分子可产生出较强的表面增强喇曼信号.同时,对该现象的产生机制也进行了理论解释.     

结晶紫、碱性品红、染料1555吸附在银胶上的表面增强喇曼散射的激发波长关系

本文通过研究在不同激发波长下吸附在银胶上的结晶紫、碱性品红、染料1555的表面增强喇曼散射散射强度的变化,分析了普通喇曼散射、表面增强喇曼散射及表面增强共振喇曼散射之间的联系与不同。     

Pt和Pd的超薄覆盖层对Ag膜表面增强喇曼散射的影响

在用化学沉积法制成的银岛膜上,蒸镀上不同厚度的Pt和Pd,测量了吡啶分子在Pt-Ag,Pd-Ag体系的表面增强喇曼散射(SERS)谱,得到SERS谱随覆盖层厚度的增加而衰减的关系曲线,并与电磁衰减理论计算的结果作了比较。此外,在两个体系都发现了新的振动谱线。我们认为它对应于吡啶在Pt和Pd上的吸附态。 关键词：     

卤化物对水扬酸分子表面增强喇曼信号的影响

研究了几种卤化物对水扬酸分子表面增强喇曼信号的影响,给出了表面增强喇曼谱(SERS)强度随卤离子浓度的变化及对时间的变化过程.并且对影响表面增强喇曼信号的机理进行了一定的分析.     

Ag涂层内凹弧形针尖增强喇曼散射效应仿真研究

设计了一种表面镀有Ag涂层且具有内凹弧度的圆锥形钨(W)针尖,运用时域有限差分法建立了针尖-球形样品结构的针尖增强喇曼散射模型,研究了针尖增强效应及参数优化配置.采用波长632.8nm光源斜入射激励方式,对模型的针尖增强喇曼散射效应进行电磁场仿真计算,获得了模型在不同光源入射角度、样品粒径、针尖-样品间距下的增强电场强度和针尖增强喇曼散射增强因子.研究结果表明:当光源入射角为72°、样品粒径约为140nm、针尖-样品间距达到2nm时可产生最大的增强因子,达到104量级.该结果为制备高增强效率的探针针尖,及其在高空间分辨率和高检测灵敏度喇曼光谱仪中的实用化提供了参考依据.     

表面增强红外付立叶变换喇曼散射

在Ag胶中对吡啶分子进行了红外表面增强付立叶变换喇曼散射研究,发现增强因子为3.4×10~4,添加少量KCL时为4.5×10~5。还对吖啶橙和罗丹明B荧光分子进行了红外付里叶变换喇曼散射测量并与可见光下的表面增强喇曼光谱进行了比较。在此基础上讨论了红外付里叶变换喇曼的优缺点和应用前景。     

银片上茜素的表面增强共振喇曼散射效应及模式标识

本文对吸附在经连续的氧化 还原循环(ORC)过程处理的银片衬底上的茜素的表面增强共振喇曼散射(SERRS)特性进行了研究,并对茜素SERRS谱中的振动模式做了标识.结果表明,吸附在经氧化.还原循环(ORC)处理的银片衬底上的茜素分子,其表面增强喇曼散射的强度,主要是由于最靠近银片的一层分子的增强,而第一层以外的分子贡献很小.也就是说,表面增强喇曼散射具有单层饱和效应.茜素在经ORC处理的银片上和在银镜上所显示的SERRS特征基本一致,其中有些振动模式存在小的频移,这与银片、银镜各自的表面特性有关.     

后向泵浦高功率掺镱光纤放大器的非弹性散射效应

 在考虑受激布里渊散射和受激喇曼散射效应的基础上,数值求解了双包层掺镱光纤放大器的速率-传输方程,分析了后向泵浦高功率掺镱光纤放大器在不同信号光线宽、光纤长度和纤芯直径下的输出特性,研究了受激布里渊散射和受激喇曼散射的抑制条件。计算结果表明:在后向泵浦方式下,若掺镱光纤长度小于0.68 m,纤芯直径大于26 μm,信号光线宽大于0.04 nm,则放大过程中的受激布里渊散射和受激喇曼散射能同时得到有效抑制。     

Zn0.76Cd0.24Se/ZnSe多量子阱的共振喇曼光谱

本文报道了在Zn0.76Cd0.24Se/ZnSe多量子阱(MQWs)中,用不同的Ar+激光线激发,观察到了共振增强的喇曼散射。首次在室温和77K的条件下,用Ar+的457.9nm谱线激发,观察到分别来自ZnSe垒层和Zn0.76Cd0.24Se阱层的限制纵光学声子模(LO)的喇曼散射,并对上述不同的光学模的起因进行了分析。     

表面增强的分子间能量转移效应的机理研究

对吸附于粗糙金属银表面的分子间能量转移效应的机理进行了研究.采用电磁理论,讨论了金属银表面对分子间能量转移速率的影响.结果表明,当能量供体(D)分子的辐射频率和能量受体(A)分子的吸收频率同时与银表面等离子体激发频率共振时,分子间非辐射的能量转移速率被增强10~3—10~4倍.采用表面增强喇曼散射(SERS)活性表面-银胶,测量了吸附的2,2菁染料单体分子和J聚集体分子的荧光光谱,观察到的J聚集体分子增强的592.4nm的荧光带是通过被加速的分子间能量转移过程而产生的,从而证实了表面增强的分子间能量转移效 关键词：     

Using surface enhanced Raman scattering to study vibrations of adsorbates on thin metallic overlayers on silver

We have studied the surface enhanced Raman scattering from molecules adsorbed on thin gold overlayers on silver island films. The Raman scattering of gold cyanide species adsorbed on gold overlayers decreases in intensity with gold overlayer thickness between 0.5 – 10 Å . This intensity decrease is consistent with a simple model which takes into account the damping of the electromagnetic resonances of the silver islands by the absorbing gold overlayer. Implications of these findings for the enhancement of Raman scattering from adsorbates on other metals deposited as overlayers on silver will be discussed.     

Raman of indigo on a silver surface. Raman and theoretical characterization of indigo deposited on silicon dioxide-coated and uncoated silver nanoparticles

Raman, surface-enhanced Raman scattering, and shell isolated nanoparticles-enhanced Raman scattering techniques were used to study the indigo–nanoparticle interaction nature. Silver nanoparticles were employed with and without a silicon dioxide spacer inert layer. The SERS spectral profile, obtained using silver nanoparticles, is different from the Raman one, which led to the proposition that the indigo–silver interaction is in the range of intermolecular interactions. SERS spectral reproducibility suggests identical organization and orientation of the analyte on the metal surface. The shell isolated nanoparticles enhanced Raman scattering spectrum of indigo, obtained by using silicon dioxide coated silver nanoparticles resulted similar to its Raman spectrum. This result indicates that the indigo structure is chemically unmodified by the silicon dioxide-coated silver surface. From the shell-isolated nanoparticles-enhanced Raman scattering experiments, the electromagnetic mechanism is proposed as the reason for the spectral enhancement. Theoretical calculations allow one to infer both the indigo–silver surface interaction nature and the orientation of indigo on the surface.     

The role of direct surface interaction in surface enhanced Raman scattering by pyridine and CO on silver

The surface enhanced Raman scattering (SERS) phenomenon due to pyridine on silver and CO on silver in ultra-high vacuum (UHV) has been compared. The study was carried out for two different kinds of silver surfaces, island films and “cold” films on island films. We have reported earlier that it was necessary to warm the samples to about 70K in order to observe the full surface enhanced Raman spectrum when the pyridine was deposited on silver island films on sapphire substrates at liquid He temperatures. We call this the effect of a “low temperature anneal” and the present work indicates that this effect is more general than we originally thought. It has also been found that island films exhibit enhanced Raman scattering for pyridine but not for CO, although “cold” films enhance the Raman scattering of both CO and pyridine. This is the first clear indication that molecular specificity may be a part of the SERS phenomenon. The interpretation of these observations depends critically on our understanding of the SERS phenomenon.     

Confinement of acoustical vibrations in a semiconductor planar phonon cavity

Extending the idea of optical microcavities to sound waves, we propose a phonon cavity consisting of two semiconductor superlattices enclosing a spacer layer. We show that acoustical phonons can be confined in such layered structures when the spacer thickness is an integer multiple of the acoustic half-wavelength at the center of one of the superlattice folded minigaps. We report Raman scattering experiments that, taking profit of an optical microcavity geometry, demonstrate unambiguously the observation of a phonon-cavity confined acoustical vibration in a GaAs/AlAs based structure. The experimental results compare precisely with photoelastic model calculations of the Raman spectra.     

聚甲基丙烯酸甲酯间隔的金纳米立方体与金膜复合结构的表面增强拉曼散射研究

金属纳米颗粒与金属薄膜的复合结构由于其局域表面等离子体和传播表面等离子体间的强共振耦合作用,可作为表面增强拉曼散射(SERS)基底,显著增强吸附分子的拉曼信号.本文提出了一种聚甲基丙烯酸甲酯(PMMA)间隔的90 nm金纳米立方体与50 nm金膜复合结构的SERS基底,通过有限元方法数值模拟,得到PMMA的最优化厚度为15 nm.实验制备了PMMA间隔层厚度为14 nm的复合结构,利用罗丹明6G (R6G)为拉曼探针分子, 633 nm的氦氖激光器作为激发光源,研究了复合结构和单一金纳米立方体的SERS效应,发现复合结构可以使探针分子产生比单一结构更强的拉曼信号.在此基础上,研究了不同浓度金纳米立方体水溶液条件下复合结构中R6G的拉曼光谱.结果表明,当金纳米立方体水溶液浓度为5.625μg/mL的条件下复合结构中R6G的拉曼信号最强,且可测量R6G的最低浓度达10~(–11) mol/L.     

Double resonant Raman scattering in nanographite films

Experimental results are presented on Raman scattering in graphite films produced by DC plasmaenhanced chemical vapor deposition from a methane-hydrogen gas mixture. Scanning electron and probe microscopy data show that, depending on substrate material and deposition time, the deposited film is either a mesoporous material consisting of graphite nanocrystallites with basal planes oriented perpendicular to the substrate surface or an atomically flat, nanometer-thick stack of graphene layers parallel to the substrate. A comparative Raman spectroscopy analysis is performed for film samples deposited on nickel and silicon substrates for 5 and 60 min, as well as for highly ordered graphite samples. The Raman spectra of the examined samples correspond to the double resonant scattering mechanism. The behavior of Raman peak position and intensity as functions of excitation wavelength suggests a high degree of structural order in the graphite films deposited on nickel for 5 min. The results obtained are used to show that the thickness of these films is 1.5 ± 0.5 nm.     

一种新基底上的C_(60)表面增强拉曼光谱研究

利用金纳米颗粒在十八胺分子的LB膜上自组装得到了一种新的表面增强拉曼光谱(SERS)活性基底。以C60分子作为这种新基底的探针分子,得到了高质量的C60SERS光谱。不但C60的振动模式增加了,而且很多模式发生了分裂,特别是一些禁戒的模式也出现在光谱中,这说明这种新基底是一种非常高效的活性基底。C60分子在新基底上的增强机制可能来自"热点"增强。     

Raman micro‐spectroscopy for quantitative thickness measurement of nanometer thin polymer films

The sensitivity of far‐field Raman micro‐spectroscopy was investigated to determine quantitatively the actual thickness of organic thin films. It is shown that the thickness of organic films can be quantitatively determined down to 3 nm with an error margin of 20% and down to 1.5 nm with an error margin of 100%. Raman imaging of thin‐film surfaces with a far‐field optical microscope establishes the distribution of a polymer with a lateral resolution of ~400 nm and the homogeneity of the film. Raman images are presented for spin‐coated thin films of polysulfone (PSU) with average thicknesses between 3 and 50 nm. In films with an average thickness of 43 nm, the variation in thickness was around 5% for PSU. In films with an average thickness of 3 nm for PSU, the detected thickness variation was 100%. Raman imaging was performed in minutes for a surface area of 900 µm². The results illustrate the ability of far‐field Raman microscopy as a sensitive method to quantitatively determine the thickness of thin films down to the nanometer range. Copyright © 2015 John Wiley & Sons, Ltd.     

Effect of boron ion implantation on the structural, optical and electrical properties of ZnSe thin films

Zinc Selenide (ZnSe) thin films were deposited onto well cleaned glass substrates using vacuum evaporation technique under a vacuum of 3×10⁻⁵ mbar. The prepared ZnSe samples were implanted with mass analyzed 75 keV B⁺ ions at different doses ranging from 10¹² to 10¹⁶ ions cm⁻². The composition, thickness, microstructures, surface roughness and optical band gap of the as-deposited and boron-implanted films were studied by Rutherford backscattering (RBS), grazing incidence X-ray diffraction, Atomic force microscopy, Raman scattering and transmittance measurements. The RBS analysis indicates that the composition of the as-deposited and boron-implanted films is nearly stoichiometric. The thickness of the as-deposited film is calculated as 230 nm. The structure of the as-deposited and boron-implanted thin films is cubic. It is found that the surface roughness increases on increasing the dose of boron ions. In the optical studies, the optical band gap value decreases with an increase of boron concentration. In the electrical studies, the prepared device gave a very good response in the blue wavelength region.     

银薄膜对光学基底表面粗糙度及光散射的影响

为了研究金属银薄膜与光学基底表面粗糙度和光散射的关系,提出了通过对光学薄膜矢量散射公式积分来获得界面粗糙度完全相关模型和完全非相关模型下其表面的总反射散射的方法.理论计算了光学基底上两种模型在不同厚度银膜下的总反射散射和双向反射分布函数.结果表明,当沉积在光学基底上的银薄膜的厚度大于80 nm后,两种模型下计算的银薄膜的表面总反射散射都等于基底的总积分散射,银薄膜能较好地复现出基底的粗糙度轮廓.实验研究表明为了复现基底的粗糙度,银薄膜的最佳厚度应在80~160 nm之间.