Epitaxial films of In2O3 have been grown on Y-stabilised ZrO2(111) substrates by molecular beam epitaxy over a range of thicknesses between 35 and 420 nm. The thinnest films are strained, but display a 'cross-hatch' morphology associated with a network of misfit dislocations which allow partial accommodation of the lattice mismatch. With increasing thickness a 'dewetting' process occurs and the films break up into micron sized mesas, which coalesce into continuous films at the highest coverages. The changes in morphology are accompanied by a progressive release of strain and an increase in carrier mobility to a maximum value of 73 cm2 V - 1 s - 1. The optical band gap in strained ultrathin films is found to be smaller th...
Abstract Control of lattice strain in epitaxial films of ABO3 perovskite oxides is crucial for moder...
The growth of micrometer sized arrays of InO islands on Y-stabilized ZrO(100) was investigated. Indi...
Precise control over the morphology of one-dimensional (1D) nanostructures is an essential step in t...
Epitaxial films of In(2)O(3) have been grown on Y-stabilised ZrO(2)(111) substrates by molecular bea...
We demonstrate that metal oxides exhibit the same relationship between lattice strain and electronic...
Reciprocal space mapping using synchrotron-based X-ray diffraction has been used to study the effect...
Thickness dependence of the strain, band gap and transport properties of epitaxial In2O3 thin films ...
Transparent conducting oxides (TCOs) combine optical transparency in the visible region with a high ...
The optical band gap of the prototypical semiconducting oxide SnO<sub>2</sub> is shown to be continu...
In this work, we report on the epitaxial growth of high-quality cubic indium oxide thick films on c-...
Thin films of In2O3 have been grown on Y-stabilised ZrO2(100) substrates by oxygen plasma assisted m...
Oxygen plasma assisted molecular beam epitaxy was used to grow thin films of In 2O 3 on α-Al 2O 3(00...
Epitaxial strain has been extensively used to control and induce new properties in complex oxide thi...
We address the issue of the local structure in an epitaxial semiconductor thin film undergoing strai...
The Poisson ratio ν of In 2O 3 has been determined by measurement of the covariation of in-plane and...
Abstract Control of lattice strain in epitaxial films of ABO3 perovskite oxides is crucial for moder...
The growth of micrometer sized arrays of InO islands on Y-stabilized ZrO(100) was investigated. Indi...
Precise control over the morphology of one-dimensional (1D) nanostructures is an essential step in t...
Epitaxial films of In(2)O(3) have been grown on Y-stabilised ZrO(2)(111) substrates by molecular bea...
We demonstrate that metal oxides exhibit the same relationship between lattice strain and electronic...
Reciprocal space mapping using synchrotron-based X-ray diffraction has been used to study the effect...
Thickness dependence of the strain, band gap and transport properties of epitaxial In2O3 thin films ...
Transparent conducting oxides (TCOs) combine optical transparency in the visible region with a high ...
The optical band gap of the prototypical semiconducting oxide SnO<sub>2</sub> is shown to be continu...
In this work, we report on the epitaxial growth of high-quality cubic indium oxide thick films on c-...
Thin films of In2O3 have been grown on Y-stabilised ZrO2(100) substrates by oxygen plasma assisted m...
Oxygen plasma assisted molecular beam epitaxy was used to grow thin films of In 2O 3 on α-Al 2O 3(00...
Epitaxial strain has been extensively used to control and induce new properties in complex oxide thi...
We address the issue of the local structure in an epitaxial semiconductor thin film undergoing strai...
The Poisson ratio ν of In 2O 3 has been determined by measurement of the covariation of in-plane and...
Abstract Control of lattice strain in epitaxial films of ABO3 perovskite oxides is crucial for moder...
The growth of micrometer sized arrays of InO islands on Y-stabilized ZrO(100) was investigated. Indi...
Precise control over the morphology of one-dimensional (1D) nanostructures is an essential step in t...