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Magnetoelastic response of La0.7Sr0.3MnO3/SrTiO3 superlattices to reversible strain
被引:32
|作者:
Dekker, M. C.
[1
]
Herklotz, A.
[1
]
Schultz, L.
[1
]
Reibold, M.
[2
]
Vogel, K.
[2
]
Biegalski, M. D.
[3
]
Christen, H. M.
[3
]
Doerr, K.
[1
,4
]
机构:
[1] IFW Dresden, D-01171 Dresden, Germany
[2] Tech Univ Dresden, Inst Struct Phys, D-01062 Dresden, Germany
[3] Oak Ridge Natl Lab, Ctr Nanophase Mat Sci, Oak Ridge, TN 37830 USA
[4] MLU Halle Wittenberg, Inst Phys, D-06120 Halle, Germany
来源:
PHYSICAL REVIEW B
|
2011年
/
84卷
/
05期
关键词:
LA0.7CA0.3MNO3;
FILMS;
THIN LA0.7SR0.3MNO3;
SPIN POLARIZATION;
MAGNETOTRANSPORT;
MAGNETORESISTANCE;
MULTILAYERS;
DEPENDENCE;
INTERFACE;
LAYERS;
D O I:
10.1103/PhysRevB.84.054463
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
The influence of an electrically controlled biaxial in-plane strain on the magnetization of superlattices of ferromagnetic La0.7Sr0.3MnO3 and SrTiO3 was studied for single-layer thicknesses of d = 1.5-13 nm. Super-lattices were grown by pulsed laser deposition on both SrTiO3(001) and piezoelectric 0.72Pb(Mg1/3Nb2/3)O-3-0.28PbTiO(3)(001), or PMN-PT(001), substrates and have been structurally characterized by x-ray diffraction (XRD) and transmission electron microscopy. Grazing-incidence XRD reveals the vertical homogeneity of the piezoelectrically controlled reversible in-plane strain, even in a 600-nm-thick superlattice containing 100 oxide interfaces. The as-grown strain is almost identical in all superlattices that are coherently grown, with small variations resulting from the partially relaxed growth of the first La0.7Sr0.3MnO3 layer on PMN-PT(001). The magnetic transition temperature decreases with the layer thickness d as a consequence of the finite layer thickness, and the strain-induced response of the magnetization changes its character from that of a long-range-ordered ferromagnet to that of a magnetically disordered (possibly electronically phase-separated) manganite. The strain response of a modified interface layer ("dead layer") of the thickness d(I) is distinguished from that of the layer's interior by its different temperature dependence, allowing an estimation of 10 angstrom < d(I) < 16 angstrom for the superlattices on PMN-PT.
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