2012
DOI: 10.1039/c2nr00039c
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Controlling magnetoelectric coupling by nanoscale phase transformation in strain engineered bismuth ferrite

Abstract: The magnetoelectric coupling in multiferroic materials is promising for a wide range of applications, yet manipulating magnetic ordering by electric field proves elusive to obtain and difficult to control. In this paper, we explore the prospect of controlling magnetic ordering in misfit strained bismuth ferrite (BiFeO(3), BFO) films, combining theoretical analysis, numerical simulations, and experimental characterizations. Electric field induced transformation from a tetragonal phase to a distorted rhombohedra… Show more

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Cited by 47 publications
(26 citation statements)
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“…10. Similar phenomena could be also observed in other materials {e.g., Bi 0.5 Na 0.5 TiO 3 [45] and BiFeO 3 [32,[49][50].…”
Section: Nature Of Giant Piezoelectricity Around R-t Phase Boundarysupporting
confidence: 52%
“…10. Similar phenomena could be also observed in other materials {e.g., Bi 0.5 Na 0.5 TiO 3 [45] and BiFeO 3 [32,[49][50].…”
Section: Nature Of Giant Piezoelectricity Around R-t Phase Boundarysupporting
confidence: 52%
“…26 The stability of the written domain structures is important for the application of ferroelectrics for memories and other applications. 33 In glycine, the domains are stable for a short time only and then their length slowly decreases to reach stable configuration or sometimes they fully disappear similar to the case of single-domain strontium-barium niobate (SBN) crystals. 34 However, the time taken for the nucleated domain to switch back after removal of the field is much slower than the intrinsic switching time.…”
Section: Resultsmentioning
confidence: 99%
“…To examine whether the enhanced electromechanical response is due to bulk intrinsic mechanisms such as electrostriction and polarization rotation, thermodynamic calculations were performed following formalism developed elsewhere, 35 as detailed in the Supplemental Material. 32 For bulk rhombohedral BFO, such calculations resulted in a spontaneous polarization of 100 μC/cm 2 , a d 33 of 21 pm/V, and a dielectric constant of 97, in good agreement with both density functional theory calculations and recent experimental measurements 32 (see also Refs.…”
mentioning
confidence: 99%