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Nano-structural characteristics and optical properties of silver chiral nano-flower sculptured thin films

机译:银手性纳米花雕刻薄膜的纳米结构特征和光学性质

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Silver chiral nano-flowers with 3-, 4- and 5-fold symmetry were produced using oblique angle deposition method in conjunction with the rotation of sample holder with different speeds at different sectors of each revolution corresponding to symmetry order of the acquired nano-flower. Atomic force microscopy (AFM) and field emission scanning electron microscopy (FESEM), were employed to obtain morphology and nano-structure of the films. Optical characteristics of silver chiral nano-flower thin films were obtained using single beam spectrophotometer with both s- and p-polarization incident light at 30° and 70° incidence angles and at different azimuthal angles (φ). Optical spectra showed both TM (TDM (transverse dipole mode) and TQM (transverse quadruple mode)) and LM (longitudinal mode) Plasmon resonance peaks. For 3- and 4-fold symmetry chiral nano-flowers the s-polarization extinction spectra obtained at different azimuthal angles did not show significant change in the Plasmon peak position while 5-fold symmetry chiral nano-flower showed a completely different behavior, which may be the result of increased surface anisotropy, so when the φ angle is changed the s-polarization response from the surface can change more significantly than that for lower symmetries. In general, for 3-, 4- and 5-fold symmetry chiral nano-flowers a sharp peak at lower wavelengths (<450 nm) is observed in the s-polarization spectra, while in addition to this peak a broad peak at longer wavelengths (i.e., LM) observed in the p-polarization spectra, which is more dominant for 70° incidence angle.
机译:使用倾斜角沉积方法,结合样品支架在每个旋转的不同扇区以不同速度旋转(对应于获取的纳米花的对称顺序),产生具有3、4和5倍对称性的银手性纳米花。 。利用原子力显微镜(AFM)和场发射扫描电子显微镜(FESEM)获得了薄膜的形貌和纳米结构。使用单光束分光光度计,在30°和70°入射角和不同方位角(φ)下,使用s偏振和p偏振入射光,可获得银手性纳米花薄膜的光学特性。光谱显示了TM(TDM(横向偶极子模式)和TQM(横向四极子模式))和LM(纵向模式)等离子共振峰。对于3倍和4倍对称手性纳米花,在不同方位角获得的s极化消光光谱在Plasmon峰位置上没有显示出显着变化,而5倍对称手性纳米花则表现出完全不同的行为,这可能这是表面各向异性增加的结果,因此,当改变φ角度时,与较低对称性相比,来自表面的s极化响应的变化可能更大。通常,对于3倍,4倍和5倍对称性手性纳米花,在s偏振光谱中观察到较低波长(<450 nm)的尖峰,而除此峰外,在较长波长处也有宽峰在p偏振光谱中观察到的LM(即LM),在70°入射角时更为明显。

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