Comparison and analysis of Mueller-matrix spectra from exoskeletons of blue, green and red Cetonia aurata

被引:13
作者
Arwin, H. [1 ]
del Rio, L. Fernandez [1 ]
Jarrendahl, K. [1 ]
机构
[1] Linkoping Univ, Dept Phys Chem & Biol, Lab Appl Opt, SE-58183 Linkoping, Sweden
关键词
Mueller-matrix ellipsometry; Scarab beetles; Chiral structures; Circular polarization; Natural photonic structures; CUTICLE; BEETLES; INSECTS; SCALES;
D O I
10.1016/j.tsf.2014.02.012
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The exoskeleton, also called the cuticle, of specimens of the scarab beetle Cetonia aurata is a narrow-band reflector which exhibits metallic shine. Most specimens of C. aurata have a reflectance maximum in the green part of the spectrum but variations from blue-green to red-green are also found. A few specimens are also more distinct blue or red. Furthermore, the reflected light is highly polarized and at near-normal incidence near-circular left-handed polarization is observed. The polarization and color phenomena are caused by a nanostructure in the cuticle. This nanostructure can be modeled as a multilayered twisted biaxial layer from which reflection properties can be calculated. Specifically we calculate the cuticle Mueller matrix which then is fitted to Mueller matrices determined by dual-rotating compensator ellipsometry in the spectral range 400-800 nm at multiple angles of incidence. This non-linear regression analysis provides structural parameters like pitch of the chiral structure as well as layer refractive index data for the different layers in the cuticle. The objective here is to compare spectra measured on C. aurata with different colors and develop a generic structural model. Generally the degree of polarization is large in the spectral region corresponding to the color of the cuticle which for the blue specimen is 400-600 nm whereas for the red specimen it is 530-730 nm. In these spectral ranges, the Mueller-matrix element m(41) is non-zero and negative, in particular for small angles of incidence, implicating that the reflected light becomes near-circularly polarized with an ellipticity angle in the range 20 degrees-45 degrees. (C) 2014 Published by Elsevier B.V.
引用
收藏
页码:739 / 743
页数:5
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