scholarly journals Theory of light reflection and transmission by a plasmonic nanocomposite slab: emergence of broadband perfect absorption

2021 ◽  
Vol 38 (5) ◽  
pp. 1442
Author(s):  
V. G. Bordo
2020 ◽  
Vol 1009 ◽  
pp. 63-68
Author(s):  
Sasmita Dash ◽  
Christos Liaskos ◽  
Ian F. Akyildiz ◽  
Andreas Pitsillides

In this work, we investigated graphene hypersurface (HSF) for the manipulation of THz waves. The graphene HSF structure is consists of a periodic array of graphene unit cells deposited on silicon substrate and terminated by a metallic ground plane. The performance of the proposed HSF is numerically analyzed. Electromagnetic parameters of HSF such as permeability, permittivity, and impedance are studied. The proposed graphene HSF has active control over absorption, reflection, and transmission of THz waves. The graphene HSF provides perfect absorption, zero reflection and zero transmission at resonance. Moreover, the graphene HSF structure has the advantage of anomalous reflection and frequency reconfiguration. Incident waves can be reflected in the desired direction, depending on the phase gradient of the HSF and the perfect absorption is maintained at all reconfigurable frequencies upon reconfiguration. The results reveal the effectiveness of the graphene HSF for the manipulation of THz waves.


2020 ◽  
Vol 28 (17) ◽  
pp. 25410
Author(s):  
Chi Zhang ◽  
Jianqi Zhang ◽  
Xin Wu ◽  
Melin Huang

2007 ◽  
Vol 53 (181) ◽  
pp. 201-210 ◽  
Author(s):  
Donald K. Perovich

AbstractAn understanding of the reflection and transmission of light by snow is important for snow thermodynamics, hydrology, ecology and remote sensing. Snow has an intricate microstructure replete with ice/air interfaces that scatter light. Spectral observations of light reflection and transmission, from 400 to 1000 nm, were made in temperate snowpacks, under cold and under melting conditions. The optical observations were made using a dual-detector spectroradiometer. One detector was placed above the snow surface to monitor the incident and reflected solar irradiance, and the second detector was placed at the base of snow cover to measure downwelling irradiance. The optical measurements were supplemented by a physical characterization of the snow, including depth, density and an estimate of grain size. In general, transmitted light levels were low and showed a strong spectral dependence, with maximum values between 450 and 550 nm. For example, a 10 cm thick snow layer reduced visible transmission (500 nm) to about 5% of the incident irradiance, and infrared transmission (800 nm) to less than 1%. Extinction coefficients were in the range 3–30 m−1, and tended to decrease slightly as the snow aged and increase as snow density increased.


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