Abstract

Eu1−xLaxTiO3−δ (x = 0, 0.3, 0.5) films were deposited in a p(Ar(96%)/H2(4%)) = 4 × 10−4 mbar atmosphere on (LaAlO3)0.3-(Sr2AlTaO6)0.7 vicinal substrates (0.1°). Reflection high-energy electron diffraction oscillation characteristics of a layer-by-layer growth mode were observed for stoichiometric and Ti-rich films and the laser fluence suited to deposit stoichiometric films was identified to be 1.25 J/cm2 independent of the La content. The variety of resulting film compositions follows the general trend of Eu-enrichment for low laser and Ti-enrichment for high laser fluence. X-ray diffraction confirms that all the films are compressively strained with a general trend of an increase of c-axis elongation for non-stoichiometric films. The surfaces of non-stoichiometric films have an increased roughness, the highest sheet resistances, exhibit the presence of islands, and are Eu3+ rich for films deposited at low laser fluence.

Highlights

  • The wide band-gap insulator (3.2 eV) SrTiO3 (STO) and the smaller band-gap black-colored insulator (1 eV) EuTiO3 (ETO) show, for example, metal-to-insulator transitions, anomalous Hall behavior[1] and high thermopower[2,3] when slightly doped on cationic sites or with oxygen vacancies. These properties are highly bound to the growth control of films3/single crystals with variable doping concentrations and stoichiometry control for metal-to-insulator transitions arising through valence change and/or band-gap closure[4] mechanisms

  • Recent advances in pulsed laser deposition (PLD) and molecular beam epitaxy techniques resulted in extended investigations especially with respect to the impact of oxygen partial pressure p(O2),[6] laser fluence,[7,8] etc., on the electric transport of the STO films and interfaces

  • ETO is another candidate for oxide electronics being isostructural to STO and to its structure similarities, very peculiar electromagnetic coupling properties have been the topic of recent years

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Summary

Introduction

2. (a) Cation ratio Eu/Ti of the deposited films as a function of laser fluence as evaluated from XPS measurements; the lines are guides for the eye.

Results
Conclusion

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