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Excitation of surface and volume plasmons in metal nanocluster by fast electrons

机译:快速激发金属纳米团簇中的表面和体积等离子体   电子

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摘要

Surface and volume plasmons excited in a metal cluster by moving electron andcorresponding inelastic scattering spectra are studied based on thehydrodynamic approach. Along with the bulk losses traditionally taken intoaccount, the surface and radiative ones are also considered as the physicalmechanisms responsible for the plasmon damping. The second and third mechanismsare found to be essential for the surface plasmons and depend very differentlyon the multipole mode order. The differential equations are obtained whichdescribe the temporal evolution of every particular mode as that one of alinear oscillator excited by the given external force, and the electron energyloss spectra are calculated. The changes in spectrum shape with the impactparameter and with the electron passage time are analyzed and found to be ingood enough agreement with the data of scanning transmission electronmicroscopy (STEM) experiments. It is shown that, in the general case, apronounced contribution to the formation of the loss spectrum is given by theboth surface and volume plasmons with low and high multipole indices. Inparticular, at long electron passage time, the integral loss spectrum which iscalculated for the free-electron cluster model contains two main peaks: a broadpeak from merging of many high-order multipole resonances of the surfaceplasmons and a narrower peak of nearly the same height from merged volumeplasmons excited by the electrons that travel through the central region of thecluster. Comparatively complex dependences of the calculated excitationcoefficients and damping constants of various plasmons on the order of theexcited multipole result in wide diversity of possible types of the lossspectrum even for the same cluster material and should be taken into account ininterpretation of corresponding electron energy loss spectroscopy (EELS)experiments.
机译:基于流体动力学方法研究了通过移动电子和相应的非弹性散射光谱在金属团簇中激发的表面和体积等离激元。除了传统上考虑的大量损耗外,表面损耗和辐射损耗也被认为是造成等离振子阻尼的物理机制。发现第二和第三种机制对于表面等离子体激元是必不可少的,并且在多极模式阶上有很大不同。获得了描述每个特定模式的时间演化的微分方程,该非线性方程是由给定外力激励的非线性振荡器之一,并且计算了电子能量损失谱。分析了频谱形状随冲击参数和电子通过时间的变化,发现与扫描透射电镜(STEM)实验的数据不够吻合。结果表明,在一般情况下,具有低和高多极指数的表面和体积等离激元都对损失谱的形成有明显的贡献。特别是,在较长的电子通过时间下,为自由电子团簇模型计算的积分损耗谱包含两个主要峰:来自表面等离子体的许多高阶多极子共振合并的宽峰和来自表面等离子体的几乎相同高度的较窄峰被行进到团簇中心区域的电子激发的合并的等离激元。即使对于相同的团簇材料,所计算出的激子的激发系数和阻尼常数相对于激发多极级的阶数的相对复杂的关系也会导致多种可能的损失谱类型,并且在解释相应的电子能量损失谱(EELS)时应予以考虑)实验。

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