Ultraviolet light emitting diode with n-ZnO:Ga/i-ZnO/p-GaN:Mg heterojunction
Introduction
ZnO based materials are potential semiconductors for high efficiency light emitting diodes (LEDs) in the blue and ultraviolet wavelength regions. The excellent physical and chemical properties of ZnO and oxide alloys, which include high exciton binding energy (60 meV) and possibility of wet etching processes, are expected to make them suitable alternative materials to nitrides in the next-generation illumination systems [1], [2]. The UV detecting devices with high responsivity have also been reported using ZnO based Schottky and p–n diodes [2], [3]. However, the difficulty in obtaining p-type ZnO films with high reproducibility and stability has limited the development of ZnO based optoelectronic devices, even though many groups have reported the fabrication of homojunction p–n diodes using p-type ZnO films [4], [5], [6], [7], [8].
The alternative approaches to the fabrication of ZnO based LEDs using p-type nitride epilayers grown on sapphire substrates have been suggested to overcome the p-type related problems in device applications [9]. The p-type GaN has the advantage for n-type ZnO epitaxy on account of the smaller lattice mismatch, same crystal structure, domain matching epitaxy growth, and technical stability. The n-type ZnO can be obtained conveniently using intrinsic and extrinsic methods due to the formation of native oxygen vacancies and incorporation of metal impurities such as Al, Ga, and In, respectively [10], [11], [12]. Among them, Ga is expected to be the most effective n-type dopant in ZnO because the covalent bond length of Ga–O (1.92 Å) is similar to that of Zn–O (1.97 Å) and Ga2O3 formed is less reactive than Al2O3 in Al doped ZnO [13]. However, the general LED structures have p–i–n stacking, where the intrinsic semiconductors are the emissive layer. In this study, various heterostructures were grown, using Mg doped GaN (GaN:Mg) epilayer as a p-layer and Ga doped ZnO (ZnO:Ga) as a n-layer, for fabrication of LED devices. The effects of the electrical properties of the ZnO grown by sputtering on the device performance were examined.
Section snippets
Experiments
ZnO films were grown on p-GaN:Mg epilayers by magnetron sputtering, and used to fabricate the n-ZnO/p-GaN heterostructure based LEDs. The p-GaN was deposited on a c-plane sapphire substrate using metalorganic chemical vapor deposition (MOCVD). A commercial ZnO (99.999%, 4 in) and 1 wt.% Ga doped ZnO targets were used as ZnO sources, and a mixture of high purity argon and oxygen at a ratio of 1:2 was used as ambient gas. The ZnO films were grown at 750 °C (high temperature, HT) and 450 °C (low
Results and discussions
In this study, various ZnO based materials such as HT n-ZnO:Ga (750 °C), LT n-ZnO:Ga (450 °C), and undoped i-ZnO (growth temperature, 450 °C) with different electrical properties were grown on p-GaN:Mg for the fabrication of p–n or p–i–n LEDs. Their electrical properties were examined using Hall measurements with the films grown directly on sapphire substrates, as shown in Table 1. When 1 wt.% Ga doped ZnO was used as a sputtering target, the ZnO:Ga film exhibited n-type semiconducting
Summary
ZnO thin films were grown on p-GaN epilayers by magnetron sputtering for fabrication of p–n heterostructure LEDs. The LEDs with HT n-ZnO:Ga/p-GaN:Mg showed non rectifying behavior due to high conductivity of n-ZnO:Ga, while the deposition of LT n-ZnO:Ga prior to the growth of HT n-ZnO:Ga led to diode characteristics. The EL emissions from these n-ZnO:Ga/p-GaN:Mg LEDs (samples 1 and 2) were mainly in the visible region, and coincided with the deep-level position of the PL results of n-ZnO:Ga
Acknowledgements
This work was supported by the KRF Grant (KRF-2008-314-D00153) and the Energy and Resources Technology Development Project from the MOCIE. This research was also financially supported by the Ministry of Knowledge Economy (MKE) and the Korea Industrial Technology Foundation (KOTEF) through the Human Resource Training Project for Strategic Technology.
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2015, Applied Surface ScienceCitation Excerpt :The diffusion of the O atoms was favorable for the formation of the native VO defects on the ZnO side surface, thereby resulting in the enhancement of the green emission of the resulting n-ZnO/p-GaN heterojunction LED. In addition, as the Ga atoms on the p-GaN side surface were prone to react with the in-diffused O atoms at an elevated annealing temperature [19], as mentioned in the literatures [20,26,27], the defect emission emerging from the formation of the Ga–O interlayer on the p-GaN side surface was thus responsible for the red emission centered at 630 nm, which was the dominant single over the broad long-wavelength emission as deconvoluted in the inset of Fig. 5(a). This red luminescence associated with the mechanism of the deep donor-deep acceptor transitions was also observed in the GaN contaminated with oxygen and heavily Mg-doped p-GaN [28–30].