Abstract

A fundamental strategy to enhance optical transmission through a continuous metallic film based on strong interference dominated by interface phase shift is developed. In a metallic film coated with a thin semiconductor film, both transmission and absorption are simultaneously enhanced as a result of dramatically reduced reflection. For a 50-nm-thick Ag film, experimental transmission enhancement factors of 4.5 and 9.5 are realized by exploiting Ag/Si non-symmetric and Si/Ag/Si symmetric geometries, respectively. These planar layered films for transmission enhancement feature ultrathin thickness, broadband and wide-angle operation, and reduced resistance. Considering one of their potential applications as transparent metal electrodes in solar cells, a calculated 182% enhancement in the total transmission efficiency relative to a single metallic film is expected. This strategy relies on no patterned nanostructures and thereby may power up a wide spectrum of energy-harvesting applications such as thin-film photovoltaics and surface photocatalysis.

Highlights

  • To explore the enhanced transmission based on strong interference dominated by interface phase shift in planar metal/semiconductor double-layered films, Si layers with thicknesses of [10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25] nm (in a 5 nm increment) on 30-nm-thick Ag layers are fabricated and experimental transmission at normal incidence in the visible range

  • Amorphous silicon (a-Si) and Ag are used as semiconductor and metal materials, respectively

  • The amorphous silicon (a-Si) is highly absorbing at visible frequencies owing to direct electronic transitions at energies above the absorption edge

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Summary

Introduction

To explore the enhanced transmission based on strong interference dominated by interface phase shift in planar metal/semiconductor double-layered films, Si layers with thicknesses of [10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25] nm (in a 5 nm increment) on 30-nm-thick Ag layers are fabricated and experimental transmission at normal incidence in the visible range

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