Abstract

Designs of multilayer antireflection coatings made from co-sputtered and low-refractive-index materials are optimized using a genetic algorithm. Co-sputtered and low-refractive-index materials allow the fine-tuning of refractive index, which is required to achieve optimum anti-reflection characteristics. The algorithm minimizes reflection over a wide range of wavelengths and incident angles, and includes material dispersion. Designs of antireflection coatings for silicon-based image sensors and solar cells, as well as triple-junction GaInP/GaAs/Ge solar cells are presented, and are shown to have significant performance advantages over conventional coatings. Nano-porous low-refractive-index layers are found to comprise generally half of the layers in an optimized antireflection coating, which underscores the importance of nano-porous layers for high-performance broadband and omnidirectional antireflection coatings.

Highlights

  • Minimizing optical reflection at dielectric interfaces is a fundamental challenge, and is vital for many applications in optics

  • A material with the required refractive index may not exist, and omni-directional and broadband antireflection characteristics are often required for applications such as solar cells or image sensors

  • Several methods exist that allow the tuning of refractive index for optical thin films

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Summary

Introduction

Minimizing optical reflection at dielectric interfaces is a fundamental challenge, and is vital for many applications in optics. Well-known refractive index profiles for antireflection coatings include the quintic or modified-quintic profiles, which are continuous functions that vary between the substrate refractive index and the index of the ambient material [5,6]. These profiles do not give the optimum profile when a finite number of layers is used. The parameter space generally includes many local minima, which makes deterministic optimization schemes that find the local minima unsuitable [7] To meet these challenges, genetic algorithms have previously been applied in order to optimize a variety of optical coatings [7,8,9,10]. The calculations consider coatings composed of co-sputtered and low-n materials and take material dispersion into account

Numerical approach
Silicon image sensor
Silicon solar cell
Findings
Conclusion
Full Text
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