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Magnetic Oxide Heterostructures: EuO on Cubic Oxides ... - JuSER

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A. Appendix<br />

A.1. Properties of EuO-related phases and cubic oxide substrates<br />

EuO is metastable and easily reacts to thermodynamically competing compounds. In Tab. A.1,<br />

we provide an overview of the most common Eu reaction products which are possibly related<br />

to EuO during synthesis.<br />

One objective of this thesis is the investigation of single-crystalline EuO epitaxially integrated<br />

on different cubic substrates providing biaxial strain, m = a S−a F<br />

a<br />

. In order to allow for a gradation<br />

of available substrates, in Tab. A.2, we compile lattice parameters and strain with respect<br />

F<br />

to single-crystalline EuO for different temperatures: at liquid helium, liquid nitrogen, room<br />

temperature, and during MBE synthesis of EuO. For the substrates used in this thesis, Fig. A.1<br />

illustrates the cubic cells of EuO relative to underlying oxide substrates with an indication of<br />

biaxial strain, m, and interface reactivity.<br />

For lattice-matched EuO growth, one may consider SrO (a = 5.161 Å, m =+0.4%) as well<br />

as Sr x Ba 1−x O, in which the cubic lattice parameter a is tunable by composition x (Lettieri<br />

et al. (2003)), 24,217 but these two are not commercially available due to their high reactivity<br />

in air and with humidity. The cubic ITO substrate allows for coherent EuO growth, yet tends<br />

to reduce its lattice constant for lower doping (e. g. 6% Sn). In this case, ITO would provide a<br />

small compressive strain with respect to EuO, if integrated epitaxially on cubic planes. Also<br />

the ITO crystals or films need to be synthesized on-site.<br />

For moderate tensile strain, comparable to Si (001), CeO 2 (a = 5.412 Å, m =+5.2%) would be<br />

an option.<br />

Among the commercially available substrates, cubic CaO (a = 4.815 Å, m = −6.3%) would<br />

be suited for a moderate compressive strain provided to EuO (001). CaO is chemically reactive<br />

with water and also carbon, which destroys the surface crystal structure immediately.<br />

Thus, we estimate its thermodynamic stability: CaO has a Gibbs free energy of formation of<br />

−636 kJ/mol which is larger than for EuO (Δ f G(EuO) ≈−500 kJ/mol). This predicts the thermodynamic<br />

stability of CaO in contact with EuO synthesis. However, during oxygen-limited<br />

EuO synthesis at elevated temperatures, the reaction CaO + 3EuO −→ Eu 3 O 4 + Ca results<br />

in a Gibbs free energy balance near zero. Thus, EuO may reduce CaO to propel its own oxidation,<br />

however the energy gain for that reaction is small which renders the reaction in the<br />

reversible regime (see Fig. 2.2). In conclusion, CaO is promising by means of its compressive<br />

strain, but chemically challenging due to its air-sensitivity and comparable thermodynamic<br />

stability with EuO.<br />

126

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