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1.
陈霞  翟翠萍 《化学研究》2014,(1):20-23,32
以氯金酸为前驱体,十二烷基硫醇和硼氢化钠分别作为稳定剂和还原剂,采用相转移法制备了单分散的金纳米粒子.将金纳米粒子通过乳液聚合的方法制备了纳米金/聚苯乙烯复合粒子.通过紫外-可见吸收光谱(UV-Vis)研究了纳米金和纳米金/聚苯乙烯复合粒子的光吸收特性,使用傅立叶变换红外光谱(FT-IR)、X射线衍射(XRD)、透射电子显微镜(TEM)和动态光散射(DLS)对产物的组成、晶体结构、形貌、以及粒径进行了表征.结果表明,复合粒子为粒径分布较窄的球形,其中的金纳米粒子为面心立方结构.热失重分析(TGA)说明制备的纳米金/聚苯乙烯复合粒子具有很好的热稳定性.  相似文献   

2.
发展了种基于汞离子(Hg2+)适配体(Aptamer)免标记金纳米粒子的动态光散射(DLS)法,用于灵敏、选择性的检测溶液中的Hg2+。Aptamer 5’-TTTCTTCTTTCTTCCCCCCTTGTTTGTTGTTT-3’与Hg2+的特异性结合使金纳米粒子失去保护,在含有100 mmol/L NaCl的缓冲溶液中发生聚集,金纳米粒子的平均水合粒径变大。在pH=7.43,110 nmol/L Aptamer,100 mmol/L NaCl,Hg2+与Probe DNA孵育时间为30 min的实验条件下,金纳米粒子水合粒径的变化值("D)与Hg2+的浓度成正比。检出Hg2+的线性范围为0.1 nmol/L~5μmol/L,检出限达0.1 nmol/L。湖水及矿泉水两种水样加标实验表明本方法能够用于实际水样中Hg2+的检测。  相似文献   

3.
针对As(Ⅲ)的检测问题,提出了一种基于适配体-金纳米粒子探针和光热-激光背向散射干涉原理的水中As(Ⅲ)的定量检测技术.结合了As(Ⅲ)适配体的金纳米粒子溶液呈现稳定的酒红色,对绿光有较强的吸收作用.采用532 nm的激光照射毛细管内的金纳米粒子溶液,由于光热效应溶液折射率发生变化,激光背向散射干涉(Back-Sca...  相似文献   

4.
纳米颗粒作为信号感应单元在化学与生物传感应用中已引起广泛关注,这些功能和金属纳米结构与光相互作用时产生的表面等离子体共振密切相关.表面增强拉曼散射(SERS),是指吸附在粗糙的金属纳米结构表面的被分析物,在光照射下其拉曼光谱获得显著增强的异常表面光学现象,近年来.SERS技术已广泛用于物质检测和生物传感等研究,在生物医学领域表现出巨大的应用潜力并取得了令人瞩目的研究成果.本文阐述了金纳米棒的制备方法、表面修饰和共轭生物分子的方法.并从金纳米棒表面增强拉曼散射的角度系统阐述基于金纳米棒表面增强拉曼散射的1D,2D,3D自组装,并介绍了近期金纳米棒表面增强拉曼散射在生物医学检测与成像中最具有代表性的应用研究.  相似文献   

5.
液相金纳米粒子非线性光散射方程的研究   总被引:5,自引:1,他引:4  
将激励光与液相金纳米粒子相互作用的运动方程表达为朗之万方程,对金纳米粒子的共振散射、2/3分频共振散射和2倍频共振散射进行了分析,较好地解释了液相金纳米粒子产生的一些非线性散射现象。  相似文献   

6.
利用可逆-加成断裂链转移聚合得到全亲水性的嵌段共聚物(PEO-b-PNIPAM), 通过"grafting to"使其接枝到金纳米粒子表面. 通过透射电子显微镜、 紫外-可见吸收光谱、 能谱分析及动态光散射研究了杂化的金纳米粒子的壳层结构及温度响应行为. 实验结果表明, 得到核壳结构的金纳米粒子, 同时其壳层具有温度响应行为. 随着温度的升高, 其流体力学半径略有减小. 在整个升温过程中, 由于外层PEO链段的抑制作用, 没有发生粒子间的聚集.  相似文献   

7.
采用3-巯基丙基三甲氧基硅烷作为联结剂,成功将单个金纳米粒子包在氧化硅壳中,制得Au@SiO2核壳纳米粒子;该复合纳米粒子形貌呈球形、单分散性较好,金纳米粒子位于氧化硅球的中心,无团聚的金纳米粒子包覆在氧化硅壳中。采用透射电镜(TEM)对样品的形貌进行了表征,通过能量散射X-射线能谱(EDX)分析了目标物的化学成分,并对所得核壳纳米粒子的光谱性质进行了研究。  相似文献   

8.
一维金纳米粒子链的制备及其光学特性研究   总被引:2,自引:0,他引:2  
在没有模板存在的条件下, 只用表面活性剂为稳定剂, 制备了一维的金纳米粒子链, 详细考察了链状结构形成时各种试剂浓度、种类及其它外部条件对纳米粒子链形成的影响. 实验发现, 在HAuCl4 浓度1~5 mmol•L-1、十二烷基磺酸钠(SDS)浓度在2~8 mmol•L-1 (小于其CMC)范围内, 温度由60 ℃ 0.5 h内升高到100 ℃, 并在升温时间内分次将还原剂加完, 反应完成后不老化立即冷却到室温, 可以获得一维金纳米粒子链. 采用紫外可见光谱(UV-Vis)、同步光散射光谱和发射光谱等手段对金纳米粒子链的光学特性进行了研究, 用高分辨透射电子显微镜(HRTEM)研究了金纳米粒子的外观和粒径分布, 结果表明制备的金纳米粒子链是错落有致的链状结构, 结节处可以观察到金原子的排列晶格, 说明金纳米粒子的链状连接不是外部分子作用的结果; 表面等离子体共振吸收峰出现红移现象, 且随着链长的增加红移越明显; 具有非常强的光散射特性, 散射光强度比浓度相同的金纳米粒子高8倍; 发射光谱中明显观察到其三级散射, 表明其具有很好的非线性光学特性. 对金纳米粒子链的形成机理进行了探讨, 认为表面活性剂烷基亲油作用和金原子的聚集作用相互竞争是链状结构形成的原因.  相似文献   

9.
氧化铁磁性纳米粒子的表面配体交换及相转移   总被引:1,自引:1,他引:0  
以苯甲醇为单一溶剂, 通过常压、高温热解乙酰丙酮铁, 制备了尺寸单分散的四氧化三铁磁性纳米粒子. 采用透射电镜(TEM), X射线衍射(XRD), 动态光散射(DLS)等方法对粒子形貌和结构进行了表征. 利用傅里叶变换红外(FT-IR)光谱和热重分析(TGA)研究了所制备纳米粒子的表面化学, 结果表明稳定四氧化三铁粒子的是苯甲酸分子, 且表面覆盖度小于20%. 所制备的磁性纳米粒子可以在室温下方便地进行表面配体交换, 从而为氧化铁磁性纳米粒子的功能化提供新的途径.  相似文献   

10.
研究了一种新型超分子纳米药物载体的制备方法及其药物释放性能. 将α-环糊精(α-CD)穿入肉桂酸改性的PEG分子链形成包含复合物(inclusion complex, IC), 通过超分子自组装成为纳米粒子. 将抗肿瘤药物阿霉素负载到纳米粒子中, 研究药物释放行为及其对肿瘤细胞的抑制效果. 以核磁共振(1H NMR)、X射线衍射(XRD)、紫外吸收光谱(UV)、动态光散射(DLS)、扫描电镜(SEM)、透射电镜(TEM)和原子力显微镜(AFM)表征了纳米粒子的结构和形貌, 用激光共聚焦显微镜(Confocal)研究了载药纳米粒子在细胞内的分布及其对肿瘤细胞的抑制效果. 结果显示超分子纳米粒子具有很好的生物相容性和药物缓释作用, 载药纳米粒子对肿瘤细胞具有很好的杀伤效果.  相似文献   

11.
分别对动态光散射粒径测量仪的入射波长、散射角度、测量池温度进行校准,并对影响测量结果准确性各因素的不确定度分量进行了评价,校准后动态光散射仪的测量结果可溯源至国家计量标准。为消除多重散射、颗粒间相互作用、颗粒粒径分布对动态光散射测量结果的影响,建立了动态光散射测量结果修正方法。其中为消除多重散射及颗粒间相互作用的影响,需采用多浓度测量或线性回归的方法得到特定浓度下的颗粒粒径;为修正颗粒粒径分布对动态光散射测量结果的影响,需先采用SEM方法准确测量颗粒粒径分布,然后根据光强加权动力学平均粒径和数量平均粒径的理论公式,得到二者之间的差异。  相似文献   

12.
A facile and sensitive immunoassay protocol for the detection of alpha-fetoprotein (AFP) was developed using gold-coated iron oxide magnetic nanoclusters and dynamic light scattering (DLS) methods. The increase in the average particle size due to AFP-mediated aggregation was measured using DLS, and the detection limit was better than 0.01 ng mL(-1).  相似文献   

13.
A one-step homogeneous DNA detection method with high sensitivity was developed using gold nanoparticles (AuNPs) coupled with dynamic light scattering (DLS) measurement. Citrate-protected AuNPs with a diameter of 30 nm were first functionalized with two sets of single-stranded DNA probes and then used as optical probes for DNA detection. In the presence of target DNA, the hybridization between target DNA and the two nanoparticle probes caused the formation of nanoparticle dimers, trimers, and oligomers. As a result, the nanoparticle aggregation increased the average diameter of the whole nanoparticle population, which can be monitored simply by DLS measurement. A quantitative correlation can be established between the average diameter of the nanoparticles and the target DNA concentration. This DLS-based assay is extremely easy to conduct and requires no additional separation and amplification steps. The detection limit is around 1 pM, which is 4 orders of magnitude better than that of light-absorption-based methods. Single base pair mismatched DNAs can be readily discriminated from perfectly matched target DNAs using this assay.  相似文献   

14.
The application of the dynamic light scattering (DLS) method for determining the size distribution of colloidal gold nanoparticles in a range of 1–100 nm is discussed. It is shown that rotational diffusion of nonspherical strongly scattering particles with sizes of larger than 30–40 nm results in the appearance of a false peak in a size range of about 5–10 nm. In this case, the uncritical application of the DLS method may yield particle volume or number size distributions different from those obtained by transmission electron microscopy. For weakly scattering particles with diameters of smaller that 20 nm, the DLS method demonstrates an additional peak of intensity distribution in the region of large sizes that is related to particle aggregates or byproduct particles rather than individual nanoparticles. Practical methods for solving the problem of false peaks are discussed. It is established that the width of the DLS distribution does not correspond to transmission electron microscopy data and is overestimated. The advantages and drawbacks of the methods are compared and it is noted that, at present, the DLS method is the only instrument suitable for nonperturbative and sensitive diagnostics of relatively slow aggregation processes with characteristic times on the order of 1 min. In particular, this method can be used to diagnose gold nanoparticle conjugate aggregation initiated by biospecific interactions on their surface.  相似文献   

15.
Multiangle dynamic light scattering (DLS) provides a better estimate of particle size distributions (PSD) than single-angle DLS. However, multiangle data treatment requires appropriate weighting of each autocorrelation measurement prior to calculation of the PSD. The weighting coefficients may be directly obtained from (i). the autocorrelation baselines or (ii). independent measurement of the average light intensity by elastic light scattering. However, the propagation of errors associated with such procedures may intolerably corrupt the PSD estimate. In this work, an alternative recursive least-squares calculation is proposed that estimates the weighting coefficients on the basis of the complete autocorrelation measurement. The method was validated through a numerical example that simulates the analysis of a polystyrene latex with a bimodal PSD and with "measurements" taken at 10 detection angles. The ill-conditioned nature of the problem determines that the "true" PSD cannot be recovered, even in the absence of errors. A sensitivity analysis was carried out to determine the effect of errors in the weighting coefficients on the PSD recoveries.  相似文献   

16.
Temperature dependent phase behavior of poly(N-isopropylacylamide) (PNIPAM) microgels in water/methanol mixtures of different composition was studied with dynamic light scattering (DLS) and small-angle neutron scattering (SANS). Using DLS, it is possible to measure the diffusion coefficient, and thus the size of particles exactly and directly; the variation of the phase transition temperature in the different solvents is also easy to detect by this method. With SANS measurements in D2O/MeOD mixtures, some of the DLS results were confirmed. Moreover, SANS measurements give valuable information on the particle structure in different solvents. The experiments were compared with the theory of competitive hydration introduced by Tanaka et al. We found a good agreement of theory and experiment, and obtained the theoretical predictions: around the transition temperature, the composition of the bound methanol along the chains is higher than that of the outer solution, while the whole methanol composition inside the gel is lower. © 2012 Wiley Periodicals, Inc. J Polym Sci Part B: Polym. Phys. 2013, 51, 1100–1111  相似文献   

17.
本文报告了用于检测单囊泡及其粒径分析的石英纳米通道电阻-脉冲分析方法. 采用圆柱形石英纳米通道可检测粒径为100~300 nm的单磷脂囊泡和直径为170~400 nm的聚苯乙烯纳米颗粒. 单囊泡和纳米颗粒的迁移可通过检测各自产生的方波电流脉冲信号, 并由此确定颗粒尺寸. 结果表明,采用石英纳米通道电阻-脉冲分析方法得到的颗粒/囊泡粒径与采用动态光散射法和扫描电子显微法得到的结果完全一致. 这种基于电子的分析方法具有快速简单的特点,所用的自制微传感器廉价耐用. 石英通道的应用还可与其它分析方法如电流分析法和荧光显微法联用,以获得生物囊泡及人工囊泡更完全的信息.  相似文献   

18.
Asymmetrical flow field-flow fractionation (AsFIFFF) was used to determine the hydrodynamic particle sizes, molar masses, and phase transition behaviour of various poly(N-isopropylacrylamide) (PNIPAM) samples synthesised by reversible addition--fragmentation chain transfer (RAFT) and conventional free radical polymerisation processes. The results were compared with corresponding data obtained by dynamic light scattering (DLS) and size exclusion chromatography (SEC). Agreement between the three methods was good except at higher molar masses, where the molar mass averages obtained by SEC were much lower than those obtained by AsFIFFF and light scattering. The aggregation of the polymers, which are thermally sensitive, was studied by DLS and AsFIFFF at various temperatures. In deionised water there was an abrupt change in the particle size due to phase separation at approximately equal to 32-35 degrees C. The critical temperatures determined by AsFIFFF were 3-5 degrees C higher than those obtained by DLS.  相似文献   

19.
以正硅酸乙酯为前驱体,聚乙烯吡咯烷酮(PVP)为聚合物改性添加剂,在碱性条件下制备氧化硅溶胶,通过小角X射线散射测量了改性溶胶的微结构参数,辅以动态光散射观测溶胶颗粒生长,研究了聚合物量、碱催化剂量和水量对溶胶颗粒度、分形特征以及流变性的影响规律.由于PVP链中强极性的分子内酰胺基团和氧化硅颗粒表面的羟基形成氢键,致使溶胶颗粒被聚合物链包裹,严重阻碍了溶胶颗粒的生长,使凝胶时间延长,流变性发生变化,同时对溶胶颗粒的微结构产生影响.  相似文献   

20.
Electrophoretic inks, which are suspensions of colorant particles that are controllably concentrated and dispersed by applied electric fields, are the leading commercial technology for high-quality reflective displays. Extending the state of the art for high-fidelity color in these displays requires improved understanding and control of the colloidal systems. In these inks, reverse micelles in nonpolar media play key roles in media and particle charging. Here we investigate the effect of surfactant structure on reverse micelle size and charging properties by synthesizing different surfactants with variations in polyamine polar head groups. Small-angle X-ray scattering (SAXS) and dynamic light scattering (DLS) were used to determine the micelle core plus shell size and micelle hydrodynamic radius, respectively. The results from SAXS agreed with DLS and showed that increasing polyamines in the surfactant head increased the micelle size. The hydrodynamic radius was also calculated on the basis of transient current measurements and agreed well with the DLS results. The transient current technique further determined that increasing polyamines increased the charge stabilization capability of the micelles and that an analogous commercial surfactant OLOA 11000 made for a lower concentration of charge-generating ions in solution. Formulating magenta inks with the various surfactants showed that the absence of amine in the surfactant head was detrimental to particle stabilization and device performance.  相似文献   

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