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Generating narrow plasmon resonances from silver nanoparticle arrays: influence of array pattern and particle spacing

机译:从银纳米粒子阵列产生窄的等离子体共振:阵列图案和粒子间距的影响

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The extinction spectra of silver nanoparticle arrays are studied using the couple dipole (CD) method, with emphasis on determined the array pattern and particle spacing which produces the narrowest plasmon resonances. All calculations refer to one and two dimensional arrays of spherical particles having radii 50 ran (or of nonspherical particles with the equivalent effective volume), and only particle spacings much larger than the particle radius are considered so that the dipole approximation is accurate. The narrowest lines in all cases occur when the incident wave vector is perpendicular to the plane of the array while the polarization vector is in the plane and along a symmetry axis which depends on the array structure. We find that the narrowest plasmon bands for square and hexagonal arrays have about the same width (about 100 meV), but that the array spacing for the square array where this occurs is smaller than that for the hexagonal array. The comparison at constant array density is closer. Much smaller widths (20 meV) occur for one dimensional arrays than for two dimensional arrays. For rectangular lattices, we find that the array spacings perpendicular to the polarization vector play a much more important role in determining the plasmon wavelength and width than do spacings parallel to the polarization vector. The evolution of spectra from a two dimensional array to a one dimensional chain is studied by considering rectangular arrays in which one spacing is very large. We find that when the large spacing is 5000 nm or more, the interactions between rows of particles is weak and extinction spectrum has a narrow peak that matches what is seen for the equivalent one dimensional chain.
机译:使用偶极偶极(CD)方法研究银纳米粒子阵列的消光光谱,重点是确定产生最窄等离子体共振的阵列模式和粒子间距。所有计算均涉及半径为50 ran的球形粒子(或等效体积的非球形粒子)的一维和二维阵列,并且仅考虑比粒子半径大得多的粒子间距,以使偶极近似准确。在所有情况下,最窄的线出现在入射波矢量垂直于阵列平面而偏振矢量在平面内并沿着取决于阵列结构的对称轴的情况下。我们发现,正方形和六边形阵列的最窄等离激元带具有大约相同的宽度(约100 meV),但发生这种情况的正方形阵列的阵列间距小于六角形阵列。在恒定阵列密度下的比较更加接近。一维阵列的宽度(20 meV)比二维阵列小得多。对于矩形晶格,我们发现垂直于偏振矢量的阵列间距在确定等离激元波长和宽度方面起着比平行于偏振矢量的间距更重要的作用。通过考虑其中一个间距非常大的矩形阵列,研究了光谱从二维阵列到一维链的演化。我们发现,当大间距为5000 nm或更大时,粒子行之间的相互作用较弱,消光光谱的峰较窄,与等效一维链的峰相匹配。

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