Manipulating light polarizations with a hyperbolic metamaterial waveguide

2015 ◽  
Vol 40 (20) ◽  
pp. 4595 ◽  
Author(s):  
Hua Zhu ◽  
Xiang Yin ◽  
Lin Chen ◽  
Zhongshu Zhu ◽  
Xun Li
Keyword(s):  
Hyperbolic Metamaterial ◽  
Metamaterial Waveguide

scholarly journals Tunable slow light in graphene-based hyperbolic metamaterial waveguide operating in SCLU telecom bands

2017 ◽  
Vol 25 (7) ◽  
pp. 7263 ◽  
Author(s):  
Anna Tyszka-Zawadzka ◽  
Bartosz Janaszek ◽  
Paweł Szczepański
Keyword(s):  
Slow Light ◽  
Hyperbolic Metamaterial ◽  
Metamaterial Waveguide

scholarly journals Rainbow Trapping in Hyperbolic Metamaterial Waveguide

CLEO: 2013 ◽  
2013 ◽  
Author(s):  
Haifeng Hu ◽  
Dengxing Ji ◽  
Xie Zeng ◽  
Kai Liu ◽  
Qiaoqing Gan
Keyword(s):  
Hyperbolic Metamaterial ◽  
Metamaterial Waveguide

scholarly journals Ultrabroad terahertz bandpass filter by hyperbolic metamaterial waveguide

2015 ◽  
Vol 23 (9) ◽  
pp. 11657 ◽  
Author(s):  
Xuetong Zhou ◽  
Xiang Yin ◽  
Tian Zhang ◽  
Lin Chen ◽  
Xun Li
Keyword(s):  
Bandpass Filter ◽  
Hyperbolic Metamaterial ◽  
Metamaterial Waveguide

scholarly journals Rainbow Trapping in Hyperbolic Metamaterial Waveguide

2013 ◽  
Vol 3 (1) ◽  
Author(s):  
Haifeng Hu ◽  
Dengxin Ji ◽  
Xie Zeng ◽  
Kai Liu ◽  
Qiaoqiang Gan
Keyword(s):  
Hyperbolic Metamaterial ◽  
Metamaterial Waveguide

scholarly journals Controlling photonic spin Hall effect by a symmetric hyperbolic metamaterial waveguide

2021 ◽  
Author(s):  
Mingxiang Gao ◽  
Wenqiong Zhang ◽  
Bin Guo
Keyword(s):  
Hall Effect ◽  
Sandwich Structure ◽  
Spin Hall Effect ◽  
Hyperbolic Metamaterial ◽  
Dielectric Matrix ◽  
Metamaterial Waveguide ◽  
Metal Type ◽  
Fill Fraction ◽  
Two Factors ◽  
Sub Wavelength

Abstract We investigate the photonic spin Hall effect (PSHE) in a symmetrical hyperbolic metamaterial (HMM) waveguide, which is constructed as an HMM/metal/HMM sandwich structure. We consider both type {\uppercase\expandafter{\romannumeral 1}} and type {\uppercase\expandafter{\romannumeral 2}} HMM in the study. We confirm that the structure of alternating sub-wavelength of plasma and dielectric or the structure of embedding plasma into a host dielectric matrix can display effective dielectric, effective metal, type {\uppercase\expandafter{\romannumeral 1}} and {\uppercase\expandafter{\romannumeral 2}} HMM under different wavelength ranges and different plasma fill fraction. This enable us to simultaneously realize type {\uppercase\expandafter{\romannumeral 1}} and type {\uppercase\expandafter{\romannumeral 2}} HMM. We show that the reflectivity ration $\vert r_{s}/r_{p} \vert$, directly related to transverse shifts generated by PSHE, greatly depends on the type and the thickness of HMM. Moreover, we find that the horizontal PSHE shifts are enhanced several times, especially in type {\uppercase\expandafter{\romannumeral 1}} structure; while the vertical PSHE shifts are significantly suppressed in both type {\uppercase\expandafter{\romannumeral 1}} and {\uppercase\expandafter{\romannumeral 2}} structure. By making the effect of metal type and thickness analysis, we further show that the impacts of these two factors on PSHE shifts are mainly subject to HMM thickness.

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