研究目的
Investigating the giant modulation of visible light scattering from achiral gold half-rings when switching between evanescent surface wave excitation produced from total internal reflection of left-handed and right-handed circularly polarized light.
研究成果
The study demonstrates a near-perfect modulation of the scattering from gold half-ring nanoantennas excited through total internal reflection of circularly polarized light, with the effect being dependent on the relative orientation of the structure and the wave vector. The research presents a fundamentally different mechanism for chiroptical responses, based on sensitivity to a phase delay between transverse and longitudinal field oscillations, not found in free-space light.
研究不足
The study is limited to the specific geometry of gold half-ring nanoantennas and their response to evanescent field excitation. The effect is dependent on the orientation of the half-ring relative to the incident wave vector, and the study does not explore other nanostructure geometries or materials.
1:Experimental Design and Method Selection:
The study involved the fabrication of gold half-ring nanoantennas using standard electron beam lithography and their characterization under evanescent field excitation produced by total internal reflection of circularly polarized light.
2:Sample Selection and Data Sources:
Arrays of gold half-ring nanoantennas with specific dimensions were fabricated and their scattering properties were measured.
3:List of Experimental Equipment and Materials:
A homebuilt inverted dark-field microscope, quartz tungsten halogen lamp, bandpass filter, planar convex lens, polarization optics, and a hyperspectral detection system were used.
4:Experimental Procedures and Operational Workflow:
The scattering from the nanoantennas was measured under different polarization states of the incident light, and the data was collected in a hyperspectral fashion.
5:Data Analysis Methods:
The scattering spectra were analyzed to determine the modulation of scattering intensity under different polarization states.
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