Niebieskikwiat D, Hueso L E, Borchers J A, Mathur N D, Salamon M B
Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA.
Phys Rev Lett. 2007 Dec 14;99(24):247207. doi: 10.1103/PhysRevLett.99.247207.
We use polarized neutron reflectometry and dc magnetometry to obtain a comprehensive picture of the magnetic structure of a series of La(2/3)Sr(1/3)MnO3/Pr(2/3)Ca(1/3)MnO3 (LSMO/PCMO) superlattices, with varying thickness of the antiferromagnetic (AFM) PCMO layers (0<or=tA<or=7.6 nm). While LSMO presents a few magnetically frustrated monolayers at the interfaces with PCMO, in the latter a magnetic contribution due to ferromagnetic (FM) inclusions within the AFM matrix is maximized at tA approximately 3 nm. This enhancement of FM moment occurs at the matching between layer thickness and cluster size, implying the possibility of tuning phase separation by imposing appropriate geometrical constraints which favor the accommodation of FM nanoclusters within the "non-FM" material.
我们使用极化中子反射测量法和直流磁强计,以全面了解一系列La(2/3)Sr(1/3)MnO3/Pr(2/3)Ca(1/3)MnO3(LSMO/PCMO)超晶格的磁结构,其中反铁磁(AFM)PCMO层的厚度不同(0≤tA≤7.6纳米)。虽然LSMO在与PCMO的界面处存在一些磁阻挫单层,但在后者中,由于AFM基质内的铁磁(FM)夹杂物导致的磁贡献在tA约为3纳米时达到最大值。这种FM矩的增强发生在层厚度与团簇尺寸匹配时,这意味着通过施加适当的几何约束来调节相分离的可能性,这些约束有利于FM纳米团簇在“非FM”材料中的容纳。