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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. 相似文献
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分子半导体组成的异质结构是染料敏化太阳能电池的主要部分,电荷转移效率的提高是太阳能转换效率的关键.在金属纳米粒子与染料分子和半导体TiO2组成的系统中,考虑半导体的晶格结构、电子波函数在晶格边界的反射及金属纳米粒子中的等离激元效应,应用密度矩阵理论研究在光激发分子作用下电荷从分子转移到半导体晶格的动力学过程,采用密度矩阵和波函数相结合的处理方案研究了分子半导体电荷转移过程中的等离激元效应.研究发现金属钠米粒子激发所产生的等离激元可以使电荷从分子到半导体的转移效率提高3个数量级,是提高电荷转移效率的有效手段,且密度矩阵理论与波函数相结合的方法使得计算分子与15 nm尺度的半导体纳米晶体间的电荷转移成为可能,理论分析了表面等离激元的增益作用对电荷转移的影响. 相似文献
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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. 相似文献
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等离激元共振能量转移指表面等离激元将俘获的能量通过偶极-偶极相互作用转移到邻近的半导体或分子等激子体系中,它是等离激元非辐射弛豫的一个通道,也可作为获取和利用等离激元共振能量的一种方式.此外,等离激元能量还可以通过热电子弛豫(非辐射)和光散射(辐射)等方式耗散.等离激元各个弛豫通道之间存在着很强的关联,相关的能量转移和电荷转移过程可以将等离激元耗散的能量输送到其他体系或转换为其他能量形式.本文主要介绍了等离激元共振能量转移和与其相关的能量和电荷转移过程(包括等离激元近场增强及耦合、远场散射、热电子弛豫等)的物理机制和动力学性质,并详细介绍了这些机制在增强光催化研究领域的最新进展. 相似文献
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表面等离激元与量子发射体间的强耦合现象通常通过散射、吸收以及荧光等远场光谱探测方法进行研究.利用高度聚焦的电子束,电子能量损失谱能够实现亚纳米尺度的局域探测,可以更加有效地研究强耦合现象.本文在理论上分别模拟了银纳米棒、介质材料以及介质层包裹银纳米棒复合结构的电子能量损失谱.得到了可以与实验结果比拟的银纳米棒表面等离激元的电子能量损失谱.在上述复合结构的电子能量损失谱中观察到了谱峰的拉比劈裂,探究了银纳米棒尺寸对拉比劈裂的影响.分别在红外、可见光波段讨论了介质层的元激发与银纳米棒偶极辐射及高阶非辐射表面等离激元模式间的强耦合现象,从损失谱的空间分布成像角度探讨了强耦合引起的杂化等离激子(plexciton)的形成.本研究对强耦合现象的进一步实验和理论研究具有指导意义. 相似文献
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表面等离激元以其独特的光学性质广泛应用于纳米尺度的局域电磁场增强、超高分辨成像及微弱光电探测.阴极荧光是电子与物质相互作用而产生的光学响应,利用电子束激发金属纳米结构能够实现局域等离激元共振,并在亚波长尺度实现对共振模式的调控,具有超高空间分辨的成像特点.阴极荧光探测通常结合扫描电子显微镜或透射电子显微镜而实现,目前己被应用于表面等离激元的探测及共振模式的分析.本文从阴极荧光物理机理出发,综述了单一金属纳米结构和金属耦合结构的等离激元共振模式阴极荧光研究进展,并总结了阴极荧光与角分辨、时间分辨以及电子能量损失谱等关键技术相结合的应用,进一步分析了其面临的关键问题,最后展望了阴极荧光等离激元研究方向. 相似文献
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研究了金属板的上下表面附近各放置一层按周期排列的电介质小球的体系的光学性质.用多重散射法计算的结果显示金属上侧的周期性排列的电介质小球可诱发金属-电介质表面上的表面等离子激元.这些表面等离子激元的存在可通过非常尖锐的吸收峰反映出来.对于无限厚的金属板,这些吸收峰的峰值位置主要与电介质小球的周期有关,且与解析理论符合得相当好.在有限厚度的金属板中,金属板的两侧表面会产生对称和反对称的两种表面等离子激元,从而使原来在无限厚的金属表面上所出现的单一频率的表面等离子激元劈裂为双频率.由于对称和反对称的表面等离子激元模式在金属板的两侧表面均有相当强的电磁场,因而它们可导致强的电磁波穿透.通过在金属板的下侧加入玻璃球层可将表面等离子激元的电磁场引导出金属,并产生透射波.用多重散射法计算的结果证实,在此体系中由表面等离子激元所引起的透射可达到相当的强度. 对该体系中的物理机理进行了详细分析,从而能够通过调节该体系中的一些参数来控制表面等离子激元出现的频率,使强吸收峰或强透射峰出现在所希望的频率上.
关键词:
表面等离子激元
吸收谱
透射 相似文献
12.
Lei Liu Feifei Lu Jian Tian Xingyue Zhangyang 《Particle & Particle Systems Characterization》2021,38(3):2000294
Since the adsorption of alkali metals is necessary for the negative electron affinity (NEA) of the photocathode, light absorption models of GaN nanowire (NW) arrays with alkali metal (Li, Na, K, and Cs) nanoparticles (NPs) modified on the NW surface based on the finite difference time domain (FDTD) method are constructed. The absorption spectra of hemispherical, spherical alkali metal NPs adsorbed on the outer surface of the NW, and spherical alkali metal embedded on the inner surface and center of the NW are studied. When the ratio of NW diameter to period (D/P) is greater than 0.5, the adsorption of alkali metal NPs cannot improve the absorption of GaN NW arrays. Alkali metal decoration can cause the absorption gain of NW arrays and optical loss of NPs, so the diameter and spacing of alkali metal NPs need to be balanced. When Li NPs are embedded in NW, plasmons can enhance the generation of electron-hole pairs, making GaN NWA obtain higher optical absorption and quantum efficiency. Therefore, the method of Li and Cs NPs embedded in GaN NW can provide a reference for the process NEA design, which will contribute to the development of the ultraviolet photocathode with high absorption characteristics. 相似文献
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Using Ohm’s law, a solution to plasmon hybridization via Kirchoff’s equations results in a simple and intuitive picture of a metal nanoparticle dimer as a capacitively coupled circuit. Calculated absorption spectra and surface charge densities show that dimers of different metallic composition support different super- and sub-radiant plasmons compared to homodimers. Strong screening of Coulomb interactions between nanoparticles of different metallic background prohibits the excitation of anti-bonding plasmons, while changes to the free electron conductivity upon a collective response result in coupled plasmon lifetimes which shift as a function of interparticle distance. Smaller separations then result in the longest lived plasmons. 相似文献
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Nonradiative electron excitation energy transfer between the molecules adsorbed by the plane conducting surface is investigated.
It is demonstrated that the mechanism with participation of surface plasmons can be efficient for energy transfer in such
system. A dependence of the energy transfer rate in the donor-acceptor adsorbate pair on the distance and anisotropy parameters
is established. The efficiencies of the direct dipoledipole and plasmon channels of energy transfer are compared. The dominating
(exceeding by 1–2 orders of magnitude the energy transfer rate in a system without conducting bodies) contribution of the
plasmon mechanism to the total energy transfer rate is detected when molecules are close to the metal surface. 相似文献
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Analytical expressions for dispersion curves of plasmons in a metal cylinder and a cylindrical cavity in metal are derived at small radii of the cylinder. The plasmon path length and the plasmon energy transfer in such structures are estimated. 相似文献
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D. N. Vasil’ev E. S. Koltsova D. A. Chubich 《Bulletin of the Lebedev Physics Institute》2010,37(3):87-88
The plasmon-exciton interaction in composite nanoparticles consisting of a metal (Au) core coated with two layers of organic materials, i.e., a monomolecular dielectric interlayer and a layer of cyanine dye J-aggregate was studied. In contrast to previously studied systems, metal in nanoobjects under consideration is at a distance of 1.2 nm from the J-aggregate, which allows maintaining the interaction of metal plasmons and J-aggregate excitons and weakening luminescence quenching at the same time. The particle morphology was studied by transmission electron and atomic-force microscopy. Bands caused by the dye J-aggregate formation on the surface were detected in the absorption spectrum of such particles. Fast dynamics (several picoseconds) of optical density variation was detected by the pump-probe method. The photoluminescence spectrum contains a narrowband characteristic of J-aggregates, which is excited due to a locally strengthened field of metal core plasmons. 相似文献
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The 1s spectrum in beryllium metal and the plasmons accompanying it have been measured by the XPS method. The analysis shows that the plasmons are created with about equal probability by direct energy loss and by the conduction electron hole coupling. 相似文献
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《Infrared physics》1985,25(5):661-664
Both stimulated emission and absorption of surface plasmons are considered in MIM (transition metal type like) junctions. The net stimulated emission coefficient (the difference between stimulated emission and stimulated absorption) and the dielectric loss (including free carrier) coefficient for surface plasmons in an Mg-Al2O3-Ni structure are calculated. Net amplification of the anti-symmetric plasma wave is predicted in the IR wavelength region. 相似文献
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石墨烯中等离激元具有特殊的光电性质,其和入射光的强烈耦合可以引起光吸收的增强.本文基于时域有限差分法和多体自洽场理论研究了等离激元对处于光学谐振腔中的石墨烯光吸收的影响.由于石墨烯中等离激元与入射光动量和能量不匹配而不能直接相互作用,因此石墨烯上施加了金属光栅结构.研究发现光栅结构能够对入射光进行动量补偿并且能够引起其下石墨烯中的电场强度产生很大程度增强,从而导致在该石墨烯结构中太赫兹等离激元和入射光发生强烈耦合而产生太赫兹等离极化激元,同时引起石墨烯光吸收的增强.希望本文能够加深对石墨烯光电特性的理解以及可以为基于石墨烯的太赫兹光电装置提供一定的理论依据. 相似文献