Giant birefringence in optical antenna arrays with widely tailorable optical anisotropy

被引:186
作者
Kats, Mikhail A. [1 ]
Genevet, Patrice [1 ,2 ,3 ]
Aoust, Guillaume [1 ,4 ]
Yu, Nanfang [1 ]
Blanchard, Romain [1 ]
Aieta, Francesco [1 ,5 ]
Gaburro, Zeno [1 ,6 ]
Capasso, Federico [1 ]
机构
[1] Harvard Univ, Sch Engn & Appl Sci, Cambridge, MA 02138 USA
[2] Texas A&M Univ, Inst Quantum Studies, College Stn, TX 77843 USA
[3] Texas A&M Univ, Dept Phys, College Stn, TX 77843 USA
[4] Ecole Polytech, Dept Phys, F-91128 Palaiseau, France
[5] Univ Politecn Marche, Dipartimento Sci & Ingn Mat Ambiente & Urbanist, I-60131 Ancona, Italy
[6] Univ Trent, Dipartimento Fis, I-38100 Trento, Italy
基金
美国国家科学基金会;
关键词
plasmonics; resonance; metasurfaces; scattering; PHASE DISCONTINUITIES; LIGHT; NANOPARTICLES; METAMATERIALS; REFLECTION; REFRACTION;
D O I
10.1073/pnas.1210686109
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
The manipulation of light by conventional optical components such as lenses, prisms, and waveplates involves engineering of the wavefront as it propagates through an optically thick medium. A unique class of flat optical components with high functionality can be designed by introducing abrupt phase shifts into the optical path, utilizing the resonant response of arrays of scatterers with deeply subwavelength thickness. As an application of this concept, we report a theoretical and experimental study of birefringent arrays of two-dimensional (V- and Y-shaped) optical antennas which support two orthogonal charge-oscillation modes and serve as broadband, anisotropic optical elements that can be used to locally tailor the amplitude, phase, and polarization of light. The degree of optical anisotropy can be designed by controlling the interference between the waves scattered by the antenna modes; in particular, we observe a striking effect in which the anisotropy disappears as a result of destructive interference. These properties are captured by a simple, physical model in which the antenna modes are treated as independent, orthogonally oriented harmonic oscillators.
引用
收藏
页码:12364 / 12368
页数:5
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