2014
DOI: 10.1002/crat.201300410
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Heteroepitaxy of Ga2(1‑x)In2xO3 layers by MOVPE with two different oxygen sources

Abstract: Ga 2(1-x) In 2x O 3 epitaxial layers have been grown on (0001) Al 2 O 3 substrates by metal organic vapour phase epitaxy (MOVPE). The process parameters were optimized and the effects related to the use of two alternative oxygenation sources like O 2 and H 2 O were studied. Different In content x [x = In/(In + Ga)] were investigated in order to determine the In solubility limit in β-Ga 2 O 3 . By using pure O 2 during the growth, the In amount detected in the layers increased linearly with the flux of In precu… Show more

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Cited by 35 publications
(33 citation statements)
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“…It is therefore unclear which structure the alloys would assume, and how this would affect stability and electronic properties. A number of papers have reported on the synthesis of such alloys [14][15][16][17][18][19][20][21][22][23][24][25] and on their crystal structure, band gaps and solubility limits. However, no consistent explanation for the experimental observations exists.…”
Section: (A)mentioning
confidence: 99%
“…It is therefore unclear which structure the alloys would assume, and how this would affect stability and electronic properties. A number of papers have reported on the synthesis of such alloys [14][15][16][17][18][19][20][21][22][23][24][25] and on their crystal structure, band gaps and solubility limits. However, no consistent explanation for the experimental observations exists.…”
Section: (A)mentioning
confidence: 99%
“…So far, most attention was concentrated on the thermodynamically stable b-Ga 2 O 3 phase, essentially for one reason: it can be grown both as a single crystal and as a thin epitaxial layer, thus enabling homoepitaxy and permitting one to lower the density of structural defects. Alloys with Al or In can modulate the b-Ga 2 O 3 bandgap, 4,5 allowing for the realization of heterostructures and the formation of a modulation doped 2D electron gas (2DEG) at the heterojunction, enabling high performance electronics. However, this phase presents also evident drawbacks, essentially due to the highly-asymmetric monoclinic structure.…”
Section: Introductionmentioning
confidence: 99%
“…At low pressures (5-20 mbar), no indium was incorporated in the layers, even at very high flows of In precursor, while at a higher pressure of 100 mbar, indium was incorporated into the layers. 2,23 To study the amount of indium that could be incorporated into β-Ga 2 O 3 thin films using TEGa and TEIn precursors, all growth parameters are kept constant except for the indium flow rate varying from 0 to 0.26 μmol/min (growth temperature 825°C and chamber pressure 5 mbar). Figure 5 shows the surface morphology of the β-(In,Ga) 2 O 3 films (0, 0.09, and 0.26 μmol/min, as a representative) measured by atomic force microscopy.…”
Section: Journal Of Applied Physicsmentioning
confidence: 99%
“…They have applications in power devices and deep UV optoelectronic devices because of their novel properties such as distinctive electrical conductivity, large breakdown voltage, and high dielectric constant. [1][2][3][4][5] To fully exhaust their potential, the formation of (Ga 1−x In x ) 2 O 3 alloys is desired to tune the bandgap and for the development of heterostructures. However, β-Ga 2 O 3 exhibits a monoclinic crystal structure with the space group C2/m and lattice parameters of a = 12.214 Å, b = 3.0371 Å, c = 5.7981 Å and a monoclinic angle of β = 103.83°, 6 whereas In 2 O 3 represents a cubic bixbyite system with the space group Ia-3 and a lattice parameter of a = 10.117 Å.…”
Section: Introductionmentioning
confidence: 99%
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