The magnetoresistance across interfaces in the itinerant ferromagnetic oxide SrRuO3 have been studied. To define appropriately the interfaces, epitaxial thin films have been grown on bicrystalline and laser-patterned SrTiO3 substrates. Comparison is made with results obtained on similar experiments using the double-exchange ferromagnetic oxide La2/3Sr1/3MnO3. It is found that in SrRuO3, interfaces induce a substantial negative magnetoresistance, although no traces of the low-field spin tunneling magnetoresistance are found. We discuss these results on the basis of the distinct degree of spin polarization in ruthenates and manganites and the different nature of the surface magnetic layer formed at interfaces
In recent decades, one of the most active and promising areas of condensed matter research has been...
The present work is concerned with the preparation, characterization and analysis of thin film heter...
Epitaxial La0.7Sr0.3MnO3/LaMnO3/SrRuO3 (LSMO/LMO/SRO) heterostructures with an LMO layer 0-35 nm thi...
The magnetoresistance across interfaces in the itinerant ferromagnetic oxide SrRuO3 have been studie...
We report on the growth and characterization of SrRuO3 single layers and SrRuO3/SrTiO3/SrRuO3 hetero...
The conducting oxide ferromagnets SrRuO3 (SRO) and LaSr0.3MnO3 (LSMO) form a Ru exchange spring at a...
In this work, we investigate electronic and magnetic phenomena in thin films and heterostructures of...
Magnetic interlayer coupling is a key ingredient in designing magnetic multilayers with functionalit...
Magnetic interlayer coupling is a key ingredient in designing magnetic multilayers with functionalit...
Interfaces between materials provide an intellectually rich arena for fundamental scientific discove...
Interfaces of ferroic oxides can show complex magnetic textures which have strong impact on spintron...
Ferromagnet/ferroelectric interface materials have emerged as structures with strong magnetoelectric...
A direct correlation is seen between the coercive field (HC) and the magnetic-field-dependent resist...
A detailed analysis of the in-plane magnetoresistance anisotropy in single orientation thin film SrR...
Orthorhombic YMnO3 (YMO) epitaxial thin films were deposited on SrTiO3 (STO) single-crystal substrat...
In recent decades, one of the most active and promising areas of condensed matter research has been...
The present work is concerned with the preparation, characterization and analysis of thin film heter...
Epitaxial La0.7Sr0.3MnO3/LaMnO3/SrRuO3 (LSMO/LMO/SRO) heterostructures with an LMO layer 0-35 nm thi...
The magnetoresistance across interfaces in the itinerant ferromagnetic oxide SrRuO3 have been studie...
We report on the growth and characterization of SrRuO3 single layers and SrRuO3/SrTiO3/SrRuO3 hetero...
The conducting oxide ferromagnets SrRuO3 (SRO) and LaSr0.3MnO3 (LSMO) form a Ru exchange spring at a...
In this work, we investigate electronic and magnetic phenomena in thin films and heterostructures of...
Magnetic interlayer coupling is a key ingredient in designing magnetic multilayers with functionalit...
Magnetic interlayer coupling is a key ingredient in designing magnetic multilayers with functionalit...
Interfaces between materials provide an intellectually rich arena for fundamental scientific discove...
Interfaces of ferroic oxides can show complex magnetic textures which have strong impact on spintron...
Ferromagnet/ferroelectric interface materials have emerged as structures with strong magnetoelectric...
A direct correlation is seen between the coercive field (HC) and the magnetic-field-dependent resist...
A detailed analysis of the in-plane magnetoresistance anisotropy in single orientation thin film SrR...
Orthorhombic YMnO3 (YMO) epitaxial thin films were deposited on SrTiO3 (STO) single-crystal substrat...
In recent decades, one of the most active and promising areas of condensed matter research has been...
The present work is concerned with the preparation, characterization and analysis of thin film heter...
Epitaxial La0.7Sr0.3MnO3/LaMnO3/SrRuO3 (LSMO/LMO/SRO) heterostructures with an LMO layer 0-35 nm thi...