A tunable infrared plasmonic polarization filter with asymmetrical cross resonator

来源 :Chinese Physics B | 被引量 : 0次 | 上传用户:CrazyDesire
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A tunable infrared plasmonic polarization filter is proposed and investigated in this paper. The filter is based on the sandwich absorption structure which consists of three layers. The top layer is an array of asymmetrical cross resonator.The middle and bottom layers are dielectric spacer and metal film respectively. By absorbing specific wavelength of the incident light perfectly, the reflection spectrum of the structure shows filter performance. The calculated results show that the absorption wavelength is strongly dependent on the length of branch of the asymmetrical cross resonator which is parallel to the light polarization and independent of the length of the vertical one. Therefore, the asymmetrical cross resonator filter structure opens the way for freely tuning the filtering wavelength for a different light polarization. We can fix a resonant wavelength(absorption wavelength) corresponding to one polarization and change the resonant wavelength for the other polarization by adjusting the corresponding branch length of the asymmetrical cross resonator, or change the two resonant wavelengths of both two polarizations at the same time. The tunable infrared plasmonic polarization filter is proposed and investigated in this paper. The top is an array of asymmetrical cross resonator. The middle and bottom layers are dielectric spacer and metal By absorbing specific wavelength of the incident light perfectly, the reflection spectrum of the structure shows filter performance. The calculated results show that the absorption wavelength is strongly dependent on the length of branch of the asymmetrical cross resonator which is parallel to the light polarization and independent of the length of the vertical one. Thus, the asymmetrical cross resonator filter structure opens the way for freely tuning the filtering wavelength for a different light polarization. the resonant wavelength for the other polarization by ad justing the corresponding branch length of the asymmetrical cross resonator, or change the two resonant wavelengths of both both polarizations at the same time.
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