Brûlé Yoann, Demésy Guillaume, Gralak Boris, Popov Evgeny
Opt Express. 2015 Apr 6;23(7):9167-82. doi: 10.1364/OE.23.009167.
An extensive numerical study of diffraction of a plane monochromatic wave by a single gold cone on a plane gold substrate and by a periodical array of such cones shows formation of curls in the map of the Poynting vector. They result from the interference between the incident wave, the wave reflected by the substrate, and the field scattered by the cone(s). In case of a single cone, when going away from its base along the surface, the main contribution in the scattered field is given by the plasmon surface wave (PSW) excited on the surface. As expected, it has a predominant direction of propagation, determined by the incident wave polarization. Two particular cones with height approximately 1/6 and 1/3 of the wavelength are studied in detail, as they present the strongest absorption and field enhancement when arranged in a periodic array. While the PSW excited by the smaller single cone shows an energy flux globally directed along the substrate surface, we show that curls of the Poynting vector generated with the larger cone touch the diopter surface. At this point, their direction is opposite to the energy flow of the PSW, which is then forced to jump over the vortex regions. Arranging the cones in a two-dimensional subwavelength periodic array (diffraction grating), supporting a specular reflected order only, resonantly strengthens the field intensity at the tip of cones and leads to a field intensity enhancement of the order of 10 000 with respect to the incident wave intensity. The enhanced field is strongly localized on the rounded top of the cones. It is accompanied by a total absorption of the incident light exhibiting large angular tolerances. This strongly localized giant field enhancement can be of much interest in many applications, including fluorescence spectroscopy, label-free biosensing, surface-enhanced Raman scattering (SERS), nonlinear optical effects and photovoltaics.
对平面金基底上单个金锥以及此类金锥的周期性阵列对平面单色波的衍射进行了广泛的数值研究,结果表明在坡印廷矢量图中会形成涡旋。它们是由入射波、基底反射波以及锥体散射场之间的干涉产生的。对于单个锥体,当沿着表面远离其底部时,散射场中的主要贡献来自于在表面激发的表面等离激元波(PSW)。正如预期的那样,它具有由入射波偏振决定的主要传播方向。详细研究了高度约为波长1/6和1/3的两个特定锥体,因为当它们排列成周期性阵列时表现出最强的吸收和场增强。虽然由较小的单个锥体激发的PSW显示出整体沿基底表面定向的能量通量,但我们表明,由较大锥体产生的坡印廷矢量的涡旋接触到折射面。此时,它们的方向与PSW的能量流方向相反,PSW随后被迫跳过涡旋区域。将锥体排列成仅支持镜面反射级次的二维亚波长周期性阵列(衍射光栅),会共振增强锥体尖端处的场强,并导致相对于入射波强度场强增强约10000倍。增强的场强烈地局限在锥体的圆形顶部。它伴随着入射光的完全吸收,且具有较大的角度容差。这种强烈局域化的巨大场增强在许多应用中可能会引起极大的兴趣,包括荧光光谱学、无标记生物传感、表面增强拉曼散射(SERS)、非线性光学效应和光伏。