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Interface-induced spontaneous positive and conventional negative exchange bias effects in bilayer La(0.7)Sr(0.3)MnO(3)/Eu(0.45)Sr(0.55)MnO(3) heterostructures
We report zero-field-cooled spontaneous-positive and field-cooled conventional-negative exchange bias effects in epitaxial bilayer composed of La(0.7)Sr(0.3)MnO(3) (LSMO) with ferromagnetic (FM) and Eu(0.45)Sr(0.55)MnO(3) (ESMO) with A-type antiferromagnetic (AF) heterostructures respectively. A tem...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5537235/ https://www.ncbi.nlm.nih.gov/pubmed/28761051 http://dx.doi.org/10.1038/s41598-017-07033-x |
Sumario: | We report zero-field-cooled spontaneous-positive and field-cooled conventional-negative exchange bias effects in epitaxial bilayer composed of La(0.7)Sr(0.3)MnO(3) (LSMO) with ferromagnetic (FM) and Eu(0.45)Sr(0.55)MnO(3) (ESMO) with A-type antiferromagnetic (AF) heterostructures respectively. A temperature dependent magnetization study of LSMO/ESMO bilayers grown on SrTiO(3) (001) manifest FM ordering (T(C)) of LSMO at ~320 K, charge/orbital ordering of ESMO at ~194 K and AF ordering (T(N)) of ESMO at ~150 K. The random field Ising model has demonstrated an interesting observation of inverse dependence of exchange bias effect on AF layer thickness due to the competition between FM-AF interface coupling and AF domain wall energy. The isothermally field induced unidirectional exchange anisotropy formed at the interface of FM-LSMO layer and the kinetically phase-arrested magnetic phase obtained from the metamagnetic AF-ESMO layer could be responsible for the spontaneous exchange bias effect. Importantly, no magnetic poling is needed, as necessary for the applications. The FM-AF interface exchange interaction has been ascribed to the AF coupling with [Formula: see text] ([Formula: see text] , coupling constant between AF spins) for the spontaneous positive hysteresis loop shift, and the field-cooled conventional exchange bias has been attributed to the ferromagnetically exchanged interface with [Formula: see text] (coupling constant between FM spins). |
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