利用银纳米立方增强效率的多层溶液加工白光有机发光二极管

金属纳米粒子的局域表面等离子体共振效应常被用于增强有机发光二极管中激子辐射强度,其增强效果与金属纳米粒子的共振波长、共振强度及其与激子之间的耦合密切相关.本文将具有较强局域表面等离子体共振效应的银纳米立方引入多层溶液加工白光有机发光二极管中提升器件性能.在传统的溶液加工有机发光二极管中,发光层主体一般具有较强的空穴传输性,因此激子主要在发光层/电子传输层界面附近复合.本文将银纳米立方掺入电子传输层中,使银纳米立方与激子之间产生充分的耦合作用,提高激子发光强度.对银纳米立方包裹二氧化硅外壳,一方面优化纳米立方与激子之间的距离,另一方面减小其对器件中电荷传输的影响.通过优化银纳米立方的浓度,多层溶液加工白光有机发光二极管的电流效率达到30.0 cd/A,是基础器件效率的2倍.另外,由于银纳米立方的等离子体共振光谱较宽,同时增强了白光中蓝光和黄光的强度,因此引入银纳米立方基本没有影响白光的色度.研究结果表明引入金属纳米粒子是提升多层溶液加工发光二极管性能的有效方法.     

金/银纳米颗粒对Eu掺杂薄膜发光特性影响的研究

本文将三种金属纳米颗粒(球形银纳米颗粒、三角形银纳米薄片和三角形金纳米薄片)分别置于Eu(TTFA)3掺杂的Su8薄膜上研究了它们对铕配合物薄膜发光的影响.结果显示,金属纳米颗粒的局域等离子体共振(LSPR)谱对薄膜发光有很好的调控作用.对于LSPR谱分别与铕配合物激发谱和辐射谱重叠较好的球形和三角形两种银颗粒,相比于未放置颗粒时薄膜的发光,放置有颗粒的发光有明显的增强,其中球形银颗粒的样品的发光增强效果更为明显.而对于LSPR谱与铕配合物激发谱和辐射谱都不重叠的三角形片状金颗粒,该颗粒对样品的发光则起到了猝灭作用.     

介质光栅/金属薄膜与银立方体复合结构的SPs研究

理论设计了介质光栅/金属薄膜与银纳米立方体复合结构,通过有限元方法数值模拟计算了该结构中的超高电场增强因子.使用442nm波长的激光作为表面等离子体的激发光源,研究不同尺寸银纳米立方体的消光谱以及不同光栅周期和厚度的反射光谱,得到的该复合结构的最优参数为:光栅周期312nm,厚度90nm,银纳米立方体70nm.在最优参数条件下,数值模拟了复合结构中的电场增强分布,介质光栅/金属薄膜与银纳米立方体复合结构由于存在局域表面等离子体和传播表面等离子体的共振耦合,使得光栅脊与银纳米立方体下顶点接触处热点的电场增强因子高达1.53×106.该复合结构产生的超高电场增强因子,有望应用于表面增强拉曼散射的研究.     

分子激发中的表面等离激元增强效应

金属纳米粒子的表面等离激元增强效应是纳米科学领域的一个研究热点.针对染料分子与金属纳米粒子的耦合系统,应用偶极-偶极近似计算分子与金属纳米粒子的库仑相互作用,并应用密度矩阵理论描述在不同极化方向的电场作用下的电荷输运过程,分析了分子与金属纳米粒子在不同相对位置下分子激发态的动力学过程,发现表面等离激元的增强效应与分子和金属钠米粒子的相对位置以及等离激元的耗散系数有密切关系,详细讨论了分子与金属纳米粒子间的耦合强度、外场的极化方向、等离激元的寿命及共振激发条件对分子激发态及表面等离激元增强的影响,分析了分子-金属纳米粒子耦合系统中表面等离激元增强效应的物理本质.     

偏振方向及结构间耦合作用对空心方形银纳米结构表面等离子体共振的影响

空心方形纳米结构能够激发更大面积的增强电场,故其可以作为衬底用于表面增强拉曼散射.应用离散偶极子近似算法研究了空心方形银纳米结构的消光光谱及其近场电场分布与入射光偏振方向之间的关系.研究表明,空心方形银纳米结构的表面等离子体共振峰不随入射光偏振方向的改变而移动,但是其表面增强电场分布却强烈地依赖于入射光的偏振方向.另外,还讨论了空心方形银纳米结构间的耦合作用对其表面等离子体共振模式的影响.结果发现,可以通过调节结构间的距离来改变结构间的耦合作用,同时改变了表面等离子体共振峰的位置.这些结果将为理解闭合纳米 关键词： 空心方形银纳米结构 表面等离子体 偏振 电场耦合     

光激发作用下分子与多金属纳米粒子间的电荷转移研究

金属纳米粒子在光激发作用下的增强作用是纳米科学领域的一个研究热点. 针对分子和多个不同位形下的金属纳米粒子在光激发下的相互作用展开了理论研究. 应用密度矩阵理论描述分子和金属纳米粒子同时激发产生表面等离激元后的电荷输运过程. 研究发现, 表面等离激元增强效应与分子和各个金属纳米粒子的相对位置有密切关系. 详细分析了金属纳米粒子间的耦合强度、分子和金属纳米粒子间的耦合强度、表面等离激元能级杂化、分子激发能和外场频率对表面等离激元增强效应的影响.     

十字形银纳米结构的表面等离子体光子学性质

本文应用离散偶极子近似方法计算了十字形银纳米结构的消光光谱及其近场电场强度分布. 研究表明相比于单根纳米棒, 十字形纳米结构能够提供更强的表面电场; 由于相邻凸起间的电场耦合作用, 当入射光的偏振方向改变时, 在十字形纳米结构的侧表面总能激发出较强的电场.另外, 本文还系统地研究了十字形纳米结构的形貌参数对其表面等离子体共振峰的影响. 这些结果将会指导十字形纳米结构的制备, 以满足其在表面增强拉曼散射中的应用.     

不同密度银纳米粒子对氧化锌基发光二极管发光的增强

采用分子束外延法制备不同密度的银纳米粒子(AgNPs)修饰的局域表面等离子体共振增强n-ZnO/iZnO/MgO/p-GaN异质结发光二极管(LEDs),并对其电学及光学性质进行表征。结果显示:LEDs中引入适当浓度的AgNPs有利于AgNPs局域表面等离子体激元与ZnO激子相耦合,可以显著提高器件的电致发光性能;随着AgNPs浓度的增加,LEDs发光增强倍数先增大后减小,分析认为这是AgNPs局域表面等离子体共振耦合增强过程和AgNPs的消光过程两者之间相互博弈而导致的结果。     

金属复合纳米粒子的局域表面等离子体特性研究

提出了一种在银层上面覆盖一层金的四棱台复合纳米结构。采用离散偶极子近似(DDA)方法,针对光激发复合金属纳米粒子的局域表面等离子体共振(LSPR)进行研究,讨论了四棱台纳米粒子金银复合结构在不同尺寸、不同混合比等条件下的消光特性及折射率灵敏度。计算结果显示,在银层厚度为50 nm的四棱台纳米粒子上覆盖金层,其折射率灵敏度不变。同时,四棱台银纳米粒子厚度的增加会使其消光峰值波长蓝移。金材料比例的增加会使金银复合纳米结构的消光峰值波长红移。当金银复合结构的纳米粒子的厚度大于自由电子的平均自由程时,其局域表面等离子体激发强度不发生变化。     

金光栅/金纳米颗粒SERS基底的设计、制备及其性能

表面等离子激元（SPP）和局域表面等离子共振（LSPR）耦合产生的电场增强显著高于单纯LSPR引起的电场增强。因此一种新型高效的表面增强拉曼散射（SERS）基底是寄希望于在一种复合基底中实现SPP-LSPR耦合获得的。基于SPP-LSPR耦合机理,提出一种针对633 nm激光使用的金光栅/金纳米颗粒SERS基底的设计思路以及光栅和纳米颗粒的具体结构参数。为了验证设计方法的正确性,利用电子束光刻法和化学合成法分别制备了具有相应几何尺寸特征的金光栅和金纳米颗粒,并将它们复合在一起得到了光栅/纳米颗粒SPP-LSPR耦合型复合SERS基底,这个基底相比仅有金纳米颗粒制备的LSPR型SERS基底,在检测R6G溶液时浓度可以降低2个数量级,增强因子是后者的72倍,实验结果和时域有限差分（FDTD）法理论拟合的结果基本一致。     

Tailoring magnetic and electric resonances with dielectric nanocubes for broadband and high-efficiency unidirectional scattering

The interference of optically induced electric and magnetic resonances in high-refractive-index dielectric nanoparticles provides a new approach to control and shape the scattering patterns of light in the field of nanophotonics. In this Letter, we spectrally tune the electric and magnetic resonances by varying the geometry of a single isolated lead telluride(Pb Te) dielectric nanocube. Then, we overlap the electric dipole resonance and magnetic dipole resonance to suppress backward scattering and enhance forward scattering in the resonance region.Furthermore, a broadband unidirectional scattering is achieved by structuring the dielectric nanocuboids as a trimer antenna.     

Humidity sensor based on localized surface plasmon resonance of multilayer thin films of gold nanoparticles linked with myoglobin

Layer-by-layer self-assembled multilayer thin films of gold nanoparticles (GNPs) linked with myoglobin (Mb) show substantial sensitivity to humidity at room temperature according to measurements of localized surface plasmon resonance (LSPR) absorption that relies on the interparticle interaction present in the film. The sensor response is reversible, with response and recovery times as low as 5 s. The sensing mechanism is as follows: as the ambient humidity changes, Mb molecules change their size, making the GNP-to-GNP spacing and thereby the interparticle interaction change; the change in the interparticle interaction causes a change in the LSPR absorption of the multilayer thin film. We found that the LSPR band of the multilayer thin film was almost insensitive to both the surrounding refractive index and the adlayer thickness, rendering the multilayer-film-based humidity sensor highly immune to ambient disturbances.     

Effects of thickness & shape on localized surface plasmon resonance of sexfoil nanoparticles

Localized surface plasmon(LSPR) resonance and sensing properties of a novel nanostructure(sexfoil nanoparticle)are studied using the finite-difference time-domain method. For the sandwich sexfoil nanoparticle, the calculated extinction spectrum shows that with the thickness of the dielectric layer increasing, long-wavelength peaks blueshift, while shortwavelength peaks redshift. Strong near-field coupling of the upper and lower metal layers leads to electric and magnetic field resonances; as the thickness increases, the electric field resonance gradually increases, while the magnetic field resonance decreases. The obtained refractive index sensitivity and figure of merit are 332 nm/RIU and 3.91 RIU~(-1), respectively. In order to obtain better sensing ability, we further research the LSPR character of monolayer Ag sexfoil nanoparticle. After a series of trials to optimize the thickness and shape, the refractive index sensitivity approximates 668 nm/RIU, and the greatest figure of merit value comes to 14.8 RIU~(-1).     

Plasmon resonances in a two-dimensional lattice of metal particles in a dielectric layer: Structural and polarization properties

The results of experimental and theoretical investigation of planar two-dimensional (2D) samples of plasmon structures are presented. The samples represent a 2D lattice of gold nanoparticles embedded in a thin dielectric layer and are studied by atomic force microscopy (AFM) and optical methods. Absorption bands associated with the excitation of various surface plasmon resonances (SPR) are interpreted. It is found that the choice of the mutual orientation of the polarization plane and the edge of the unit cell of the 2D lattice determines the spectral position of the lattice surface plasmon resonance (LSPR) related to the lattice period. It is shown that the interaction of p- and s-polarized light with a 2D lattice of nanoparticles is described by the dipole–dipole interaction between nanoparticles embedded in a medium with effective permittivity. Analysis of the spectra of ellipsometric parameters allows one to determine the amplitude and phase anisotropy of transmission, which is a consequence of the imperfection of the 2D lattice of samples.     

Localized Surface Plasmon Resonance of Cu@Cu2O core-shell nanoparticles: Absorption, Scattering and Luminescence

By co-deposition via RF-Sputtering and RF-PECVD methods and using Cu target and acetylene gas, we prepared Cu@Cu₂O core-shell nanoparticles on the a-C:H thin film at room temperature. Mie absorption of Cu cores, scattering from Cu₂O shell and luminescence that rises from carrier transfer in Cu@Cu₂O interface were employed to fit the whole range of visible extinction spectrum of these core-shells. From simulation it was found that scattering and luminescence have an important effect on the energy, width and shape of LSPR absorption peak. Shift of LSPR peak is more affected by the dielectric coefficient of shell than Cu core size particularly for Cu core diameter above 4 nm. Also, the LSPR absorption peak is damped by decreasing Cu core size and dielectric coefficient of shell. The energy of LSPR absorption peak is independent of shell thickness and host dielectric coefficient. The LSPR peak is damped by increasing shell thickness and host dielectric coefficient too. The scattering contribution in extinction spectra was affected more by shell size than dielectric coefficient. These points are important for detection techniques based on LSPR peak.     

Nondipole optical scattering from liquids and nanoparticles

Nondipolar contribution to optical scattering in liquids and nanoparticle suspensions has been discerned for the first time from the dominant electric dipole scattering by assigning the observed polarization and azimuthal angular distribution of scattered polarized light to pure magnetic dipole and/or electric quadrupole radiation and ruling out other (the impurity of laser polarization, multiple scattering, optical activity, and optical anisotropy) explanations. The observed scattering has potential use in the optical study of nanoparticles.     

LED梯度折射率封装结构的蒙特卡罗模拟

针对封装胶中掺杂纳米颗粒以及采用梯度折射率的LED封装模式,用蒙特卡罗方法模拟光在胶体中的传播,分析散射系数对透光率的影响.结果表明,透光率随散射系数增大而减小.对于固定的封装层数,各层均采取最佳折射率值时,透光率可以达到最大.梯度折射率值逐渐减小的多层纳米掺杂封装结构,透光率高于传统的封装模式,能够提高LED的出光效率.     

Optical properties of composite thin films containing silver nanoparticles

Absorption and reflection of electromagnetic radiation by a composite thin film consisting of a transparent dielectric matrix with inclusions of metal nanoparticles of radius much less than the wavelength were theoretically investigated based on the Maxwell–Garnett model. The absorption, reflection, and transmission of optical radiation in such a dielectric composite film were analyzed using effective optical parameters for the refractive index and absorption coefficient that depended on the nanoparticle size.     

Collective plasmon resonances in monolayers of metal nanoparticles and nanoshells

The collective plasmon resonances in a monolayer formed by metal or metal-dielectric nanoparticles with dipole or quadrupole single-particle resonances are theoretically and experimentally studied. The extinction, scattering, and absorption spectra are calculated using an exact many-particle solution for the system of interacting particles. With increasing surface density of particles in the monolayer, the dipole resonance is suppressed, and the spectrum of the collective system is determined by the quadrupole plasmon only. It is shown that the selective suppression of the long-wavelength extinction band is caused by the collective suppression of the dipole scattering mode, whereas the short-wavelength absorption spectrum of the monolayer differs little from the single-particle spectrum. Using dark-field light and atomic force microscopy, the kinetics of self-assembling of nanoshells is studied. It is shown that the universal linear relation between the relative shift of the wavelength of the collective quadrupole resonance and the relative increment of the refractive index of the surrounding medium is implemented.     

Electro-optical properties of dilute solutions of flexible molecules ; the wormlike chain model

A theory of propagation and scattering of light in dilute solutions of flexible chain molecules is developed. The solvent is represented as a continuous isotropic dielectric medium. The polymer molecules are modelled as dielectric objects which may have an anisotropic dielectric tensor. The theory, applied to the wormlike chain model, represents the polymer molecules as flexible cylinders of constant cross section and with an isotropic internal dielectric constant. The increment in the refractive index of the solution and the isotropic and anisotropic light scattering intensities due to the presence of the chain molecules are derived. The numerical results of our model for the depolarization ratio as a function of the contour length and the persistence length of the polymer and of the refractive index of the solvent are presented and compared with the corresponding results for the popular bond additive approximation (BAA). It is found that the differences between our model and this approximation are due to the neglect of intramolecular dipole-induced dipole interactions in the BAA.