journal article text

Electric-Field Control of Magnetism in Co<sub>40</sub>Fe<sub>40</sub>B<sub>20</sub>/(1-x)Pb(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>‑xPbTiO<sub>3</sub> Multiferroic Heterostructures with Different Ferroelectric Phases

Abstract

Electric-field control of magnetism in multiferroic heterostructures composed of Co<sub>40</sub>Fe<sub>40</sub>B<sub>20</sub> (CoFeB) and (1-x)­Pb­(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)­O<sub>3</sub>-xPbTiO<sub>3</sub> (PMN-xPT) with different ferroelectric phases via changing composition and temperature is explored. It is demonstrated that the nonvolatile <i>looplike</i> bipolar-electric-field-controlled magnetization, previously found in the CoFeB/PMN-xPT heterostructures with PMN-xPT in the rhombohedral (R) phase around the morphotropic phase boundary (MPB), also occurs for PMN-xPTs with both R phase (far away from MPB) and monoclinic (M) phase, suggesting that the phenomenon is the common feature of CoFeB/PMN-xPT multiferroic heterostructures for PMN-xPT with different phases. The magnitude of the effect changes with increasing temperature and volatile bipolar-electric-field-controlled magnetization with a <i>butterflylike</i> behavior occurs when the ferroelectric phase changes to the tetragonal phase (T). Moreover, for the R-phase sample with x = 0.18, an abrupt and giant increase of magnetization is observed at a characteristic temperature in the temperature dependence of magnetization curve. These results are discussed in terms of coupling between magnetism and ferroelectric domains including macro- and microdomains for different ferroelectric phases. This work is helpful for understanding the phenomena of electric-field control of magnetism in FM/FE multiferroic heterostructures and is also important for applications

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