2021
DOI: 10.1088/1367-2630/ac04c7
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Differentiation between strain and charge mediated magnetoelectric coupling in La0.7Sr0.3MnO3/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(001)

Abstract: Magnetoelectric (ME) coupling in La0.7Sr0.3MnO3/Pb(Mg1/3Nb2/3)0.7Ti0.3O3 (LSMO/PMN–PT (001)) has been probed in the past years to identify the underlying mechanism behind it. PMN–PT, which is well known for its excellent piezoelectric properties, also exhibits ferroelectricity. This motivates our interest to differentiate which effect is dominant for this ‘voltage control of magnetism’. Here, we present results for the ME coupling at different temperatures: 300 K and 80 K. In this article we discuss and explai… Show more

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Cited by 4 publications
(3 citation statements)
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“…Conversely, a positive voltage will lead to a depletion of electrons in magnetite and cause the magnetisation to increase. For other systems, such as the commonly investigated La 2/3 Sr 1/3 MnO 3 (LSMO), the effect of charge accumulation and depletion is opposite to the one discussed here, as the Mn-3d orbital is less than half filled for LSMO [39]. The polarisation coupling is dependent on the polarisation of PMN-PT with applied electric field and thus anti-symmetric regarding the sign of the electric field, in contrast to the strain coupling discussed above.…”
Section: Discussionmentioning
confidence: 56%
“…Conversely, a positive voltage will lead to a depletion of electrons in magnetite and cause the magnetisation to increase. For other systems, such as the commonly investigated La 2/3 Sr 1/3 MnO 3 (LSMO), the effect of charge accumulation and depletion is opposite to the one discussed here, as the Mn-3d orbital is less than half filled for LSMO [39]. The polarisation coupling is dependent on the polarisation of PMN-PT with applied electric field and thus anti-symmetric regarding the sign of the electric field, in contrast to the strain coupling discussed above.…”
Section: Discussionmentioning
confidence: 56%
“…Neutron reflectometry facilitates structural characterization of multilayered materials by probing their nuclear and magnetic depth profiles at device-relevant spatial scales, enabling the study of hidden interfaces in a broad range of nanostructured and thin film systems. [1][2][3][4][5][6][7][8][9][10][11] Leveraging the interaction of spin-polarized neutrons with magnetic moments, polarized neutron reflectometry (PNR) is particularly well-suited to detecting magnetic interfacial phenomena, [12][13][14][15][16] such as the magnetic proximity effect. Proximity coupling to a magnetic material induces magnetic order near the interface of an otherwise non-magnetic system, making it a promising pathway for magnetizing topological insulators (TIs) without introducing magnetic dopants.…”
mentioning
confidence: 99%
“…[5][6][7][8][9] Multiferroic heterostructures composed by ferromagnetic and ferroelectric phases are natively able to realize E-field controlling of magnetism attributed to the strain induced magnetoelectric (ME) coupling. [10][11][12][13][14] Motived by this idea, a series of cases have been explored to study the E-field manipulation magnetism, such as LSMO/PNN-PT, [15][16][17][18] YIG/PMN-PT [19][20][21] and Fe 3 O 4 / PZN-PT, 22 which verify the feasibility of E-field tuning ME coupling. However, most of these multiferroic heterostructures are prepared using physical methods by depositing ferromagnetic films directly on bulk single piezoelectric substrates, which is difficult to be integrated with traditional silicon-based semiconductor industry.…”
mentioning
confidence: 99%