Abstract

InGaN light emitting diodes (LED) structure with an embedded 1/4λ-stack nanoporous-GaN/undoped-GaN distributed Bragg reflectors (DBR) structure have been demonstrated. Si-heavily doped GaN epitaxial layers (n+-GaN) in the 12-period n+-GaN/u-GaN stack structure are transformed into low refractive index nanoporous GaN structure through the doping-selective electrochemical wet etching process. The central wavelength of the nanoporous DBR structure was located at 442.3 nm with a 57 nm linewidth and a 97.1% peak reflectivity. The effective cavity length (6.0λ), the effective penetration depth (278 nm) in the nanoporous DBR structure, and InGaN active layer matching to Fabry-Pérot mode order 12 were observed in the far-field photoluminescence radiative spectra. High electroluminescence emission intensity and line-width narrowing effect were measured in the DBR-LED compared with the non-treated LED structure. Non-linear emission intensity and line-width reducing effect, from 11.8 nm to 0.73 nm, were observed by increasing the laser excited power. Resonant cavity effect was observed in the InGaN LED with bottom nanoporous-DBR and top GaN/air interface.

Highlights

  • Gallium nitride (GaN) materials have considerable in optoelectronic devices such as light-emitting diodes (LEDs), laser diodes (LD)[1], and vertical cavity surface emitting lasers (VCSEL)[2]

  • High reflectivity in the NP-distributed Bragg reflectors (DBR) was demonstrated which matched to the PL emission wavelength and the cavity length of the InGaN active layer

  • The effective cavity length, the penetration depth in NP-DBR structure, the InGaN active layer matched to a Fabry-Pérot mode, and the narrowing divergent angle were analyzed from the far-field PL radiative spectra

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Summary

Introduction

Gallium nitride (GaN) materials have considerable in optoelectronic devices such as light-emitting diodes (LEDs), laser diodes (LD)[1], and vertical cavity surface emitting lasers (VCSEL)[2]. Large lattice mismatch and low refractive index different of the stack structures are the challenges for the epitaxial DBR structures with long epitaxial growth time. The AlInN/GaN DBR structure[12,13] is lattice matched to GaN material, but the growth of AlInN layer remains a challenge in InGaN-based LED structures. To realize the high reflectivity with less pairs of stack structure, the air-gap/GaN DBR structures with large refractive index different had been fabricated through selectively anodized processe[14,15], and thermal decomposition techniques[16,17,18]. Nanoporous GaN material has been reported as an effective low refractive index for the DBR structure applications[21,22,23]. Optical and electrical properties of the InGaN LED structure with and without nanoporous DBR structure were analyzed in detail

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