Structural, magnetic and electronic properties of pulsed-laser-deposition grown SrFeO 3− δ thin films and SrFeO 3− δ /La 2/3 Ca 1/3 MnO 3 multilayers
Perret, EdithUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Sen, KaushikUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Khmaladze, JarjiUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Mallett, Benjamin P. P.University of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Yazdi-Rizi, MeghdadUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Marsik, PremyslUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Das, SaikatUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Marozau, IvanUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland
Uribe-Laverde, Miguel AngelUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland - Present affiliation: Applied Physics and Mathematics Group, Faculty of Engineering, Universidad de La Sabana, Chía, Colombia
Andrés Prada, R. deUniversity of Fribourg, Department of Physics and Fribourg Center for Nanomaterials, Switzerland - Department of Physics, Stockholm University, Albanova University Center, Stockholm, Sweden
Journal of Physics: Condensed Matter. - 2017, vol. 29, no. 49, p. 495601
English
We studied the structural, magnetic and electronic properties of ${\rm SrFeO}_{3- \delta}$ (SFO) thin films and ${\rm SrFeO}_{3-\delta}$ /${\rm La}_{2/3}$ ${\rm Ca}_{1/3}$ MnO3 (LCMO) superlattices that have been grown with pulsed laser deposition (PLD) on ${\rm La}_{0.3}$ ${\rm Sr}_{0.7}$ ${\rm Al}_{0.65}$ ${\rm Ta}_{0.35}$ ${\rm O}_{3}$ (LSAT) substrates. X-ray reflectometry and scanning transmission electron microscopy (STEM) confirm the high structural quality of the films and flat and atomically sharp interfaces of the superlattices. The STEM data also reveal a difference in the interfacial layer stacking with a SrO layer at the LCMO/SFO and a LaO layer at the SFO/LCMO interfaces along the PLD growth direction. The x- ray diffraction (XRD) data suggest that the as grown SFO films and SFO/LCMO superlattices have an oxygen-deficient ${\rm SrFeO}_{3-\delta}$ structure with I4/ mmm space group symmetry ($\delta\leqslant 0.2$ ). Subsequent ozone annealed SFO films are consistent with an almost oxygen stoichiometric structure ($\delta \approx 0$ ). The electronic and magnetic properties of these SFO films are similar to the ones of corresponding single crystals. In particular, the as grown ${\rm SrFeO}_{3- \delta}$ films are insulating whereas the ozone annealed films are metallic. The magneto-resistance effects of the as grown SFO films have a similar magnitude as in the single crystals, but extend over a much wider temperature range. Last but not least, for the SFO/LCMO superlattices we observe a rather large exchange bias effect that varies as a function of the cooling field.