Abstract

Nano-engineering III-nitride semiconductors offers a route to further control the optoelectronic properties, enabling novel functionalities and applications. Although a variety of lithography techniques are currently employed to nano-engineer these materials, the scalability and cost of the fabrication process can be an obstacle for large-scale manufacturing. In this paper, we report on the use of a fast, robust and flexible emerging patterning technique called Displacement Talbot lithography (DTL), to successfully nano-engineer III-nitride materials. DTL, along with its novel and unique combination with a lateral planar displacement (D2TL), allow the fabrication of a variety of periodic nanopatterns with a broad range of filling factors such as nanoholes, nanodots, nanorings and nanolines; all these features being achievable from one single mask. To illustrate the enormous possibilities opened by DTL/D2TL, dielectric and metal masks with a number of nanopatterns have been generated, allowing for the selective area growth of InGaN/GaN core-shell nanorods, the top-down plasma etching of III-nitride nanostructures, the top-down sublimation of GaN nanostructures, the hybrid top-down/bottom-up growth of AlN nanorods and GaN nanotubes, and the fabrication of nanopatterned sapphire substrates for AlN growth. Compared with their planar counterparts, these 3D nanostructures enable the reduction or filtering of structural defects and/or the enhancement of the light extraction, therefore improving the efficiency of the final device. These results, achieved on a wafer scale via DTL and upscalable to larger surfaces, have the potential to unlock the manufacturing of nano-engineered III-nitride materials.

Highlights

  • III-nitride semiconductors have a crucial place in today’s optoelectronic and electronic devices[1]

  • One key parameter to establish the performance of an light-emitting diodes (LEDs) is the external quantum efficiency (EQE), which represents the ratio of the number of charge carriers injected into the device to the number of photons emitted by the LED

  • The EQE is given by the product of the internal quantum efficiency (IQE) and light extraction efficiency (LEE)

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Summary

Introduction

III-nitride semiconductors have a crucial place in today’s optoelectronic and electronic devices[1]. The EQE is given by the product of the internal quantum efficiency (IQE) and light extraction efficiency (LEE). In III-nitride materials, where layers are grown on foreign substrates such as sapphire and silicon due to the limited availability and large cost of native substrates, the relatively high densities of defects generated during growth can have a dramatic impact on the IQE. The relatively large refractive index of IIInitride materials seriously limits the amount of light that can be extracted from the LED as the majority of photons will be trapped within the structure by total internal reflection.

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