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1.
叶通  高云  尹彦 《物理学报》2013,62(12):127801-127801
采用聚碳酸酯模板和电化学沉积法制备基于金纳米棒的Raman场增强衬底, 制备的金纳米棒直径大约36 nm, 长约1 μm, 测试结果显示其共振吸收峰的位置约为540 nm. 比较了谐振和非谐振条件下的场增强情况, 并确定了场增益系数, 结果显示谐振激光激发下的增益比非谐振情况下提高了7.36倍. 本研究相对于前人的工作取得了如下进展: 一是讨论了谐振模式与非谐振模式下的金纳米棒的场增益系数, 利用谐振波长的激光激发金纳米棒, 进一步提高了场增益; 二是消除了聚碳酸酯模板分子的荧光背底, 使其在表面增强 Raman 散射方面的应用进一步变得可行. 关键词: 金纳米棒 表面增强Raman散射 聚碳酸酯模板  相似文献   

2.
ZnO纳米棒的拉曼和发光光谱研究(英文)   总被引:1,自引:0,他引:1  
本文对采用湿化学方法合成的ZnO纳米棒样品的拉曼光谱和发光光谱进行了研究。由扫描电镜结果可知,合成的ZnO纳米棒具有很好的尺寸发布均匀性,直径在30 nm左右,长度大于1微米。采用显微拉曼光谱技术,得到了632.8 nm波长激发的拉曼光谱,并和体相样品的拉曼光谱进行了对比分析;由325 nm激光波长激发得到的荧光光谱可知样品具有很好的紫外发光性质。  相似文献   

3.
用改进的化学气相沉积方法和溶液掺杂方法制备了掺Bi双包层石英基光纤. 测试了掺Bi光纤预制棒切片的吸收光谱和掺Bi光纤在特定波长下的吸收系数,在不同波长的激光激发下, 研究了掺Bi光纤的近红外荧光光谱. 掺Bi光纤在976 nm激光激发下,其荧光光谱范围在1000---1400 nm之间, 荧光峰的峰值位于1140 nm附近,半高宽约为130 nm;在793和808 nm激光激发下得到了 1000---1700 nm的超宽带近红外荧光,半高宽超过250 nm.通过对掺Bi光纤预制棒切片进行900 ℃ 保温1 h的热处理后,发现在808 nm激光 激发下预制棒切片的荧光强度增加了近4倍.研究结果表明,具有超宽带荧光特性的双包层掺Bi光纤 有望作为超短脉冲激光器和可调谐激光器的增益介质.  相似文献   

4.
采用模板合成以及溶胶凝胶方法制备了金纳米棒核/二氧化硅壳(GNR@SiO2)纳米复合粒子,探讨了这种新型纳米复合结构的可控制备、光谱性质、细胞毒性和细胞成像。通过紫外可见分光光度计、透射电镜、共聚焦显微镜对样品进行表征,结果表明:通过对反应时间的调控,获得的纳米复合粒子的二氧化硅壳层厚度可以控制在20~30nm。由于二氧化硅壳层的存在,大大提高了金纳米棒的稳定性,同时降低了金纳米棒的细胞毒性;此外,由于二氧化硅壳层具有良好的化学修饰作用,因此可以将荧光探针分子标记在二氧化硅壳层表面,修饰后的纳米复合粒子可以通过细胞内吞作用进入细胞,从而实现细胞内的光学成像。因此,该纳米粒子复合材料在生物传感、细胞成像以及光热治疗等方面有着良好的应用前景。  相似文献   

5.
采用钛酸四丁酯醇热技术制备了TiO2纳米晶溶胶,透射电子显微镜(TEM)照片显示其为粒径小于10nm的类球形形貌。该纳米晶在最大激发波长375nm激发下,在450nm处产生稳定的强荧光。不同浓度TiO2纳米晶的荧光光谱和吸收光谱表明,该发光带不仅受粒子量子尺寸效应的影响还与带内缺陷能级和表面态的电子跃迁有关,是三者共同作用的结果。以硫酸奎宁在激发波长313nm的荧光量子产率0.55为标准,测得TiO2纳米晶在不同激发波长下的荧光量子产率。结果表明,TiO2纳米晶在激发波长330~370nm范围内有较高的荧光量子产率(约为0.20),远高于文献报道值(10-3数量级)。据此,TiO2纳米晶有望成为一种有前途的无机纳米荧光探针。  相似文献   

6.
利用飞秒脉冲激光激发Cu掺杂ZnO纳米棒,研究其特有的非线性光学性质和激发机制。在激发波长为750 nm的荧光光谱中,二次谐波峰非常弱,几乎可以忽略,存在非常强的激子发光峰和Cu掺杂导致缺陷发光峰。激发强度的增大会导致这两个发光峰强度呈非线性增大,激子发光峰位产生明显红移,而缺陷发光峰位没有变化。进一步增大激发强度,缺陷发光峰强度会出现饱和甚至有所下降,而激子发光峰强度持续增大。当激发波长增加到760 nm时,从样品的荧光光谱可以清楚地识别到二次谐波峰和激子发光峰以及缺陷发光峰并存。随着激发波长的进一步增加,二次谐波强度不断增大,而激子发光峰和缺陷发光峰的强度却随之下降。当激发波长为790 nm和800 nm时,未发现激子发光峰和缺陷发光峰,非线性光谱以二次谐波为主导。研究结果表明,通过选择合适的激发波长和激发强度,可以实现发光颜色的转变,使得Cu掺杂ZnO纳米棒在全光显示方面具有潜在的发展前景。  相似文献   

7.
由飞秒激光驱动的非线性光学显微镜技术在医学组织成像中具有很多独特的优势,包括多种成像模态、高对比度、高分辨率和无标记的深层光学切片能力等.由于缺乏波长可灵活调谐的飞秒激发光源,导致在多模态成像的同时难以兼顾每种模态的对比度,从而制约了非线性光学显微镜在医学诊断中的广泛应用.本文采用基于自相位调制光谱选择的光纤激光光源,获得了中心波长在990—1110 nm范围内可调谐的高能量飞秒脉冲,并用于驱动非线性光学显微镜.采用990 nm的飞秒脉冲,通过双光子激发荧光和二倍频对胃组织成像,进一步结合图像拼接技术成功获得了胃组织的双模态大视场图像;利用1110 nm的飞秒脉冲,实现了无标记自发荧光多倍频显微镜技术,同时高效激发了胃组织的双光子激发荧光、三光子激发荧光、二倍频和三倍频信号,获得了胃组织的多模态图像.  相似文献   

8.
将经硫辛酸修饰的铕纳米颗粒和蛋白质固定在石英玻璃表面或胶原蛋白隔离的石英玻璃表面,研究蛋白质对纳米铕岛膜荧光的增强作用.研究结果发现,在275nm激发波长下,铕纳米岛膜的荧光光谱与铕纳米颗粒溶液的荧光性质相似,且微量蛋白质的加入可以使铕纳米岛膜的荧光强度增强,但被石英玻璃片吸附后,铕纳米岛膜以及铕-蛋白质体系的荧光发射峰的位置由378.8nm红移至420nm,且胶原蛋白隔离铕纳米岛膜和滴加微量BSA蛋白质的荧光光谱相似,但荧光强度没有发生明显变化.  相似文献   

9.
利用波长为800nm的单光束飞秒激光对水溶液中的金纳米棒颗粒进行了稳定地二维光捕获.通过测量金纳米棒的散射谱研究了光阱中金纳米棒之间的耦合相互作用.比较光阱中只有单个金纳米棒被捕获和两个金纳米棒同时被捕获时的散射谱.结果表明,当两个金纳米棒同时被光阱捕获时,金纳米棒之间相互排斥,存在一定的间隔,该间隔使得两个金纳米棒之间没有发生表面等离子耦合相互作用.该实验结果为金纳米棒的光操纵及其在生物分子探测等领域的研究提供技术指导及实验参考.  相似文献   

10.
二维纳米棒的布朗运动可以用平移扩散和转动扩散运动来描述.提出了一种基于去偏振-偏振图像的动态光散射(DIDLS)测量方法,通过分析纳米棒布朗运动的平移扩散和转动扩散在偏振激光入射下产生的垂直-垂直和垂直-水平偏振动态光散射信号,测量了纳米棒的尺寸和尺寸分布.研究了连续测量的偏振动态光散射信号图像间的相关系数函数,通过两次反演,计算出纳米棒的长度以及长径比,进而得到颗粒的二维尺度分布.分析了不同入射激光波长对测量结果的影响,提出自相关函数的基线值可以作为信噪比的判据.采用650,780,905 nm三种波长对直径为20 nm、长度为300 nm的纳米金棒进行了测量,得到了纳米金棒的平均尺寸和尺寸分布.  相似文献   

11.
Diffusion dynamics of gold nanoparticles (GNPs) was studied by fluorescence correlation spectroscopy (FCS). The fluorescence was studied by exciting the particles by green laser (532 nm), which is far from longitudinal plasmon band of nanorods. Transmission electron microscope (TEM) and UV-Vis-NIR spectrometer were used to characterize the gold nanoparticles. Despite their low quantum yields, GNPs possess the native fluorescence. The excellent antiphotobleaching behavior of gold nanorods leads to prospects of using FCS for its detailed studies. Using FCS, dynamic information can be extracted from the fluorescence fluctuations in the system by autocorrelation function. Maximum entropy method (MEMFCS) was used to identify the number of distinct components present in the system. The particle sizes obtained from FCS were found to be higher (by few orders of magnitude) compared to TEM analysis. This might be due to the possible contributions from cetyltrimethyl ammonium bromide (CTAB) capping in the system.  相似文献   

12.
反胶束软模板法合成PANI/TiO2纳米棒复合材料及其性能研究   总被引:1,自引:0,他引:1  
以阳离子表面活性剂十六烷基三甲基溴化胺(CTAB)形成的反胶束为模板,制备了一系列不同纳米TiO2含量的PANI/TiI2纳米复合材料.利用FTIR,UV-Vis,TG,TEM和荧光光谱等方法对产物进行了结构表征和性能研究.探讨了反胶束体系中PANI/TiO2复合纳米棒形成的自组装机理.结果表明:复合材料主要为直径30~40 nm,长约400 nm的PANI/TiO2复合纳米棒,二氧化钛纳米粒子与聚苯胺大分子之间存在强的相互作用,并对复合材料的热稳定性起到提高作用,PANI/TiO2纳米复合材料在紫外和可见光区域均有吸收,并在416 nm处激发产生荧光,荧光强度随着掺杂TiO2含量的提高得到了较大的增强.通过PANI/TiO2纳米棒复合材料中的激子离化和电荷传输过程探讨了PANI/TiO2的荧光量子效率和荧光强度增加的机理.  相似文献   

13.
We investigate the dependence of the size parameter in the Mie scattering theory on the near-field enhanced Raman scattering properties for high dielectric constant ZnO nanorods grown randomly by PLD (pulsed laser deposition). High Raman signals of Rhodamine 6G (R6G) at 532 nm excitation wavelength were observed with nanorods of 400 nm average diameter. This experimental result was explained theoretically by the size parameter described in the Mie scattering theory, not by surface plasmon polaritons. This was also confirmed by the near-field distribution calculated by the FDTD (Finite-Difference Time Domain) method. The ZnO nanorods with 400 nm average diameter can detect as low as 1 μM of R6G. This near-field enhancement factor is equivalent to that with 10-nm-thick gold-coated ZnO nanorods (nanoshells) with an average core diameter of 100 nm. Controlling the diameter of bare ZnO nanorods is effective for obtaining large enhancement factors without an additional process of gold thin film coating on them.  相似文献   

14.
We investigated the plasmonic resonance enhanced two-photon photopolymerization (PETPP) using the isolated chemical synthesized gold nanorods for fabrication of polymer/metal nanocomposites. The isolated gold nanorods with the plasmonic resonance band around 750 nm covered by photoresist were irradiated by a femtosecond laser with the wavelength of 780 nm. The PETPP trigged by the plasmonic resonance enhancement of gold nanorods was localized only in the distance smaller than 30 nm from the surface of gold nanorods, which matched the distance of plasmonic resonant enhanced field of the gold nanorod. The shapes of obtained polymer/gold nanocomposites were changed from the “dumbbell” to the “ellipsoid” with the increase of laser irradiating intensity used for PETPP. This study would provide a potential method for fabricating the plasmonic nanomaterials and nanostructures of polymer/metal nanocomposites, which could be expected to be applied in the emerging fields such as nanophotonics, nanobiosensor, nanolithography.  相似文献   

15.
The synthesis and characterisation of gold nanorods have been carried out by reduction of the gold salt HAuCl4. This has been done using a single reducing agent, acetylacetone, rather than the two reducing agents, sodium borohydride and ascorbic acid, normally required by standard wet chemistry methods of gold nanorod formation. Using this novel method, the nanorods were synthesised at several different pH values which were found to greatly affect both the rate at which the nanorods form and their physical dimensions. The concentrations of acetylacetone and silver nitrate used relative to the gold salt were found to alter the aspect ratio of the nanorods formed. Rods with an average length of 42 nm and an aspect ratio of 4.6 can be easily and reproducibly formed at pH 10 using this method. Nanorods formed under optimum conditions were investigated using TEM. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.  相似文献   

16.
采用电化学方法制备出悬浮胶体金纳米棒。在室温下测得其紫外 可见吸收光谱和荧光发射光谱。结合准静电场理论与散射理论对金纳米棒的光学特性进行了数值模拟。计算结果表明,由于金纳米棒形状的各向异性,吸收截面与散射截面均出现两个共振峰,分别对应于横截方向与长轴方向的表面等离子共振。对于几何形状一定的金纳米棒,在外围介质介电常数从1 5增加到2 5的过程中,两个共振吸收峰均增强并非线性红移。然而对于散射光谱,短波方向的共振峰线性红移,强度变化微弱;长波方向的共振峰减弱并非线性红移。  相似文献   

17.
In this work, gold nanobones with the length from 50 to 70 nm were synthesized by a seed-mediated method. The plasmonic optical properties and the roles of gold seed amount in regulating the negative curvatures of the end surfaces of the gold nanobones have also been studied. Compared with the gold nanorods, a new middle surface plasmon resonance (SPR) peak appears in the absorption spectra due to the negative curvatures on the end surfaces of the gold nanobones. What is more, the surface enhanced Raman scattering (SERS) activities of gold nanobones are much stronger than that of gold nanorods. By controlling the amount of the gold seed, the wavelength of the middle SPR peak can be adjusted between 560 and 650 nm, and the corresponding negative curvature of the end surfaces could also be fine tuned. When the amount of gold seed reaches saturation, the end surfaces of nanobones have the strongest negative curvature, which results in the greatest SERS activity. This improved SERS has been attributed to the negative curvature-induced formation of the antenna dimers. The orientation of plasmon coupling between the antenna dimers is perpendicular to the nanobones. Thus, the hot spots at the ends of nanobones could always be created when the excitation beam polarization is either parallel or perpendicular to the nanobones. This negative curvature-dependent SERS enhancement lays the foundation for the extensive application of gold nanobones in SERS.  相似文献   

18.
This report describes the development of a facile method for the synthesis of cross‐linked proteins with gold nanoclusters (CP‐GNC). The synthesis reaction is completed within 15 min at 97 °C. The synthesized CP‐GNC are characterized by using UV–vis absorption, fluorescence, X‐ray photoelectron spectroscopy, and transmission electron microscopy. CP‐GNC are approximately 100 nm in diameter and 700 nm in length, whereas AuNCs within the nanorods are approximately 6 nm in size. These materials are highly fluorescent with quantum yield of 7.2% and can be absorbed onto and release from bacterial cells in a pH‐dependent and reversible manner. The recent data show that CP‐GNC can be a useful, new tool with potential applications in fluorescent cell imaging and antibiotic targeting.  相似文献   

19.
Min Li  Linyong Qian 《光谱学快报》2017,50(10):585-590
Gold nanorods with the longitudinal plasmonic resonance peak position up to 1200?nm are prepared using an improved seedless synthetic technique. In this method, dopamine is employed as the weak reducer, whereas cetyltrimethylammonium bromide and sodium oleate are used as the binary surfactant mixture. Gold nanorods produced at various amounts of silver nitrate and hydrochloric acid were characterized by visible-near-infrared spectroscopy and scanning electron microscopy. Results show that the sizes, length-to-width aspect ratios, and the corresponding longitudinal surface plasmon resonance peaks of the synthesized gold nanorods can be tuned by altering the silver nitrate and hydrochloric acid amounts. The present method provides a new procedure for fabrication of gold nanorods with a broad range of plasmonic resonance peaks, which has a great potential for applications such as photothermal therapy and sensing.  相似文献   

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