Abstract

Investigation was made of the optical response of metal-dielectric stacks-based cavity structures embedded with graphene microheaters for the purpose of perfect absorption. The absorber configuration exploits the Ge2Sb2Te5 (GST) phase changing medium, and the effects of different parametric and operational conditions on the absorption spectra were explored. The refractive indices of GST layers can be manipulated by the external electrical pulses applied to microheaters. The amplitude and duration of electrical pulses define the crystallinity ratio of the used GST mediums. The results revealed achieving perfect absorption (> 99%) in the visible and infrared (IR) regimes of the electromagnetic spectrum upon incorporating two thin GST layers of different thicknesses (in the stack) in the amorphous state. The proposed configuration showed the capability of introducing independent transition state (amorphous and/or crystalline) for each GST layer—the visible regime could be extended to the IR regime, and the perfect absorption peak in the IR regime could be broadened and red-shifted. It is expected that the structure would find potential applications in active photonic devices, infrared imaging, detectors and tunable absorbers.

Highlights

  • Investigation was made of the optical response of metal-dielectric stacks-based cavity structures embedded with graphene microheaters for the purpose of perfect absorption

  • Microheating systems have been of significant importance in various need-based miniaturized photonic devices owing to exhibiting high Joule heating performance—the ability of providing adequate heat in minuscule

  • This figure exhibits that the increase in the thickness of the upper GST layer, as shown by the dashed arrow in the figure, results in significant broadening of the resonance absorption in the visible regime with a perfect absorption (> 99%)

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Summary

Introduction

Investigation was made of the optical response of metal-dielectric stacks-based cavity structures embedded with graphene microheaters for the purpose of perfect absorption. Investigation of the electromagnetic behavior of metal-dielectric stacks-based cavity systems attracted significant attention by the R&D community toward realizing perfect absorption in the range extended from the visible light to the infrared (IR) ­regime[1,2,3,4]. This is because of their ability to provide scalable and cost-effective schemes to devise photonic components for varieties of technological a­ pplications[5]. Microheating systems have been of significant importance in various need-based miniaturized photonic devices owing to exhibiting high Joule heating performance—the ability of providing adequate heat in minuscule

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