Domain structure of epitaxial SrRuO3 thin films -: art. no. 174411

被引:38
作者
Herranz, G
Sánchez, F
Fontcuberta, J
García-Cuenca, MV
Ferrater, C
Varela, M
Angelova, T
Cros, A
Cantarero, A
机构
[1] CSIC, Inst Ciencia Mat Barcelona, Bellaterra 08193, Barcelona, Spain
[2] Univ Barcelona, Dept Fis Aplicada & Opt, E-08028 Barcelona, Spain
[3] Univ Valencia, Inst Ciencia Mat, E-46071 Valencia, Spain
关键词
D O I
10.1103/PhysRevB.71.174411
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Growth of multidomains in epitaxial thin-film oxides is known to have a detrimental effect on some functional properties, and, thus, efforts are done to suppress them. It is commonly accepted that optimal properties of the metallic and ferromagnetic SrRuO3 (SRO) epitaxies can only be obtained if vicinal SrTiO3 (001) (STO) substrates are used. It is believed that this results from the suppression of multidomain structure in the SRO film. Here we revise this important issue. Nanometric films of SRO have been grown on STO(001) vicinal substrates with miscut (theta v) angles in the similar to 0.04 degrees-4 degrees range. Extensive structural analysis by x-ray-reciprocal space maps and mu-Raman spectroscopy indicates that single-domain, orthorhombic, SRO films are already obtained on the almost singular (theta(V) approximate to 0.1 degrees) substrate, and, thus, substrates with large miscut angles are not required to grow twin-free films. In spite of this, transport properties are found to be optimized for films grown on vicinal substrates (theta(V) >= 2 degrees). We claim that this is the result of the change of the growth mode and the resulting film morphology rather than the change of the domain structure. These findings drive the attention to the relevance of the growth mechanism at the initial stages of film growth, and we discuss its implications in other areas of oxide epitaxies. Moreover, we show that in clamped epitaxies on cubic substrates, in spite of isotropic biaxial substrate-induced strains, films may have an in-plane orthorhombic symmetry which results from the internal degree of freedom defined by rotations of the oxygen octahedrons.
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