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Temperature Dependence of Ultrathin Mixed-Phase Ga2O3 Films Grown on the α-Al2O3 Substrate via Mist-CVD

TLDR
In this paper , a hot-wall mist chemical vapor deposition (mist-CVD) method has been shown to be effective for the growth of pure α-and β-phase Ga2O3 thin films on the α-Al 2O3 substrate.
Abstract
Alpha (α)- and beta (β)-phase gallium oxide (Ga2O3), emerging as ultrawide-band gap semiconductors, have been paid a great deal of attention in optoelectronics and high-performance power semiconductor devices owing to their ultrawide band gap ranging from 4.4 to 5.3 eV. The hot-wall mist chemical vapor deposition (mist-CVD) method has been shown to be effective for the growth of pure α- and β-phase Ga2O3 thin films on the α-Al2O3 substrate. However, challenges to preserve their intrinsic properties at a critical growth temperature for robust applications still remain a concern. Here, we report a convenient route to grow a mixed α- and β-phase Ga2O3 ultrathin film on the α-Al2O3 substrate via mist-CVD using a mixture of the gallium precursor and oxygen gas at growth temperatures, ranging from 470 to 700 °C. The influence of growth temperature on the film characteristics was systematically investigated. The results revealed that the as-grown Ga2O3 film possesses a mixed α- and β-phase with an average value of dislocation density of 1010 cm–2 for all growth temperatures, indicating a high lattice mismatch between the film and the substrate. At 600 °C, the ultrathin and smooth Ga2O3 film exhibited a good surface roughness of 1.84 nm and an excellent optical band gap of 5.2 eV. The results here suggest that the mixed α- and β-phase Ga2O3 ultrathin film can have great potential in developing future high-power electronic devices.

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Journal ArticleDOI

Heteroepitaxial Growth of an Ultrathin β-Ga2O3 Film on a Sapphire Substrate Using Mist CVD with Fluid Flow Modeling

TL;DR: In this article , the authors used a simple solution-processed and nonvacuum mist CVD method to grow a heteroepitaxial β-Ga2O3 thin film at 700 °C using a Ga precursor and carrier gases such as argon and oxygen.
Journal ArticleDOI

Temperature-dependent Schottky diode behavior of Ni Schottky contacts to α-Ga2O3 film epitaxially grown on sapphire substrate

TL;DR: In this paper , Ni Schottky contacts on α-Ga2O3 epitaxial layers were fabricated on a c-plane sapphire substrate and explored their currentvoltage (I-V) characteristics dependence on temperature spanning over a wide temperature range of 100 −425K.
Journal ArticleDOI

Characteristics of Vertical Ga2O3 Schottky Junctions with the Interfacial Hexagonal Boron Nitride Film

TL;DR: In this paper , the authors presented the device properties of a Ni-gallium oxide (Ga2O3) Schottky junction with an interfacial hexagonal boron nitride (hBN) layer.
References
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Journal ArticleDOI

The Scherrer Formula for X-Ray Particle Size Determination

TL;DR: An exact derivation of the Scherrer equation is given for particles of spherical shape, values of the constant for half-value breadth and for integral breadth being obtained in this article, and various approximation methods which have been used are compared with the exact calculation.
Journal ArticleDOI

III. Dislocation densities in some annealed and cold-worked metals from measurements on the X-ray debye-scherrer spectrum

TL;DR: In this article, two basic equations are derived for deducing the dislocation density in powdered materials from the particle size and strain breadth measured from the Debye-Schemer spectrum.
Journal ArticleDOI

Heteroepitaxy of Corundum-Structured α-Ga2O3 Thin Films on α-Al2O3 Substrates by Ultrasonic Mist Chemical Vapor Deposition

TL;DR: In this paper, the α-Ga2O3 films have narrow fullwidths at half maximum (FWHMs) in their X-ray diffraction curves, for example, about 60 arcsec.
Journal ArticleDOI

Preparation of highly conductive, deep ultraviolet transparent β-Ga2O3 thin film at low deposition temperatures

TL;DR: In this article, tin doped Ga 2 O 3 films were deposited on Al 2 O3 (0001) substrates by the pulsed laser deposition method, and the films underwent a crystalline phase transition, accompanied by an abrupt decrease in conductivity.
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