2016
DOI: 10.1103/physrevb.94.100101
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Coupling of bias-induced crystallographic shear planes with charged domain walls in ferroelectric oxide thin films

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Cited by 10 publications
(8 citation statements)
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References 36 publications
(17 reference statements)
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“…To determine the as-grown polarization direction of the BFO film, we measured the displacements of the Fe ions with respect to the Bi sublattice for each unit cell in the atomic resolution STEM image using our in-house computing code (Figure 1d). [22] As the image intensity of HAADF image directly correlates to the total atomic number in the atomic column, in Figure 1d the brighter spots are the columns of Bi atoms (purple dots) while the weaker ones are Fe atoms (brown dots). Here, the spontaneous polarization direction (denoted by the yellow arrow) is antiparallel to the direction of the Fe displacement (denoted by blue arrows).…”
Section: Characterization Of the Initial Statementioning
confidence: 98%
“…To determine the as-grown polarization direction of the BFO film, we measured the displacements of the Fe ions with respect to the Bi sublattice for each unit cell in the atomic resolution STEM image using our in-house computing code (Figure 1d). [22] As the image intensity of HAADF image directly correlates to the total atomic number in the atomic column, in Figure 1d the brighter spots are the columns of Bi atoms (purple dots) while the weaker ones are Fe atoms (brown dots). Here, the spontaneous polarization direction (denoted by the yellow arrow) is antiparallel to the direction of the Fe displacement (denoted by blue arrows).…”
Section: Characterization Of the Initial Statementioning
confidence: 98%
“…22 Presently, high-resolution and scanning TEM techniques allow for observation of individual atomic displacements and, hence, give information about the internal CDW structure. With these techniques, CDWs were documented in single crystals of LiNbO 3 , 27 YMnO 3 , 28 and (Ca,Sr) 3 Ti 2 O 7 , 29,30 thin films of BiFeO 3 , 8,[31][32][33] PbTiO 3 , 34 and PZT, [35][36][37][38][39][40] and ceramics of BiFeO 3 , 41 (K,Na)NbO 3 , 42 TmMnO 3 , 43 and LuMnO 3 . 43 TEM techniques, supplemented by analyses of the energy losses of electrons (EELS) were employed recently to detect elemental components of the material in the vicinity of CDWs.…”
Section: Cdw Observationsmentioning
confidence: 99%
“…43 TEM techniques, supplemented by analyses of the energy losses of electrons (EELS) were employed recently to detect elemental components of the material in the vicinity of CDWs. 30,[38][39][40][41] Other methods were also in use: scanning electron microscopy for observations of the intersections of CDWs with etched surfaces of LiNbO 3 crystals, 44 high-resolution X-ray photoemission electron microscopy to visualize and characterize conducting DWs in ErMnO 3 , 45 low-energy electron microscopy (electron backscattering) to image CDWs in LiNbO 3 crystals. 46 High-resolution TEM studies have provided crucial information about the widths of domain walls.…”
Section: Cdw Observationsmentioning
confidence: 99%
“…We argue that this occurs, most probably, through the successive formation of ferroelectric nuclei (nanodomains) with an opposite polarization orientation, which gain in their quantity and size with increasing number of electrical pulses, as schematically depicted in Figure 2c. The nuclei formation might be preferentially initiated at the defect sites, 18,19 i.e., grain boundaries (because of the polycrystalline film) and the bottom and top interfaces of the ferroelectric. Following this interpretation, the succession of gate pulses will generate nanodomains up to a critical point, at which the polarization reversal of the entire grain occurs.…”
Section: Resultsmentioning
confidence: 99%