Built-in electric field induces polarization rotation in bilayer BiFeO3/(Ba,Sr)TiO3 thin films

JOURNAL OF ALLOYS AND COMPOUNDS

卷:812

Article

Razumnaya, G.¹  Mikheykin, A. S.¹  Stryukov, D., V²  Anokhin, A. S.²  Pavlenko, A., V²  Shirokov, V. B.^1,2  Kaliteevski, M. A.³  Mezzane, D.⁴  Lukyanchuk, I⁵ 

[1] Southern Fed Univ, Fac Phys, Rostov Na Donu 344090, Russia

[2] Russian Acad Sci, Southern Sci Ctr, Pr Chekhova 41, Rostov Na Donu 344006, Russia

[3] ITMO Univ, Kronverkskiy Pr 49, St Petersburg 197101, Russia

[4] Cadi Ayyad Univ, LMCN, Marrakech 40000, Morocco

[5] Univ Picardy Jules Verne, LPMC, F-80080 Amiens, France

关键词: Thin films;    Bismuth ferrite;    Barium-strontium titanate;    Crystal structure;    Polarization control;   

DOI  :  10.1016/j.jallcom.2019.152164

来源: Elsevier

【 摘 要 】

The crystal structure of BiFeO3/Ba(x)Sci(1-x)TiO(3) (BFO/BST) heterostructures with x = 0.2, 0.6 and 0.8, grown on single-crystal MgO (001) substrate was investigated by x-ray diffraction and Raman spectroscopy in order to determine the influence of mismatch-induced strains and spontaneous polarization in BST buffer layers on BFO layers. The lattice parameter of the BFO layers was shown to decrease with increasing concentration of Ba ions, despite the increasing in-plain lattice parameters of tetragonal unit cells of BST layers. The rhombohedral angle of the crystal structure of BFO layers demonstrates an increase towards the ideal cubic perovskite structure with the appearance of the built-in electric field, induced by the spontaneous polarization in buffer layers. This result provides a remarkable tool for the control of polarization in BFO layers and other ferroelectric films in general, by changing the built-in electric field from ferroelectric buffer layer without changing a single crystal substrate. (C) 2019 Elsevier B.V. All rights reserved.

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