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In its most general form, the magnetoelectric effect (ME) denotes any coupling between the magnetic and the electric properties of a material. The first example of such an effect was described by Wilhelm Röntgen in 1888, who found that a dielectric material moving through an electric field would become magnetized. A material where such a coupling is…
History, Microscopic origin & Linear magnetoelectric effect
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electric effect magnetic magnetoelectric material polarization displaystyle coupling linear field symmetry piezoelectric materials first also general magnetization magnetoelastic interaction properties
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| the bond length between magnetic ions | instance of | This interaction depends on details of the crystal structure | 0.80 | text |
| the angle formed by the bonds between magnetic | instance of | This interaction depends on details of the crystal structure | 0.80 | text |
| ligand ions | instance of | This interaction depends on details of the crystal structure | 0.80 | text |
| Magnetoelectric effect | related to Flexomagnetoelectric effect | Magnetically | 0.60 | section |
| Magnetoelectric effect | related to Flexomagnetoelectric effect | This | 0.60 | section |
| Magnetoelectric effect | related to Flexomagnetoelectric effect | It | 0.60 | section |
| Magnetoelectric effect | related to Flexomagnetoelectric effect | Usually | 0.60 | section |
| Magnetoelectric effect | related to Flexomagnetoelectric effect | Lifshitz | 0.60 | section |
| Magnetoelectric effect | related to Flexomagnetoelectric effect | FME | 0.60 | section |
| Magnetoelectric effect | related to General phenomenology | If | 0.60 | section |
| Magnetoelectric effect | related to General phenomenology | Differentiating | 0.60 | section |
| Magnetoelectric effect | related to General phenomenology | Here | 0.60 | section |
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