Evolution of magnetic order in multiferroic Pb(Fe2/3W1/3)O3‐BiFeO3 solid solution. Issue 9 (4th May 2021) - Li, Haijuan
Abstract: Multiferroic materials have attracted much interest in the last decade due to both the intriguing fundamental science and the potential applications in spintronics and magnetoelectric data storage devices. In this work, we have investigated and discussed the evolution of the magnetic properties of the multiferroic (1‐ x )Pb(Fe2/3 W1/3 )O3 ‐ x BiFeO3 solid solution ((1‐ x )PFW‐ x BFO, x = 0, 0.025, 0.05, 0.075, 0.1 and 0.15). The magnetic phase diagram is established based on the magnetic measurement results, which reveals six magnetically ordered states on the PFW‐rich side of the solid solution. The origins of the complex evolution of magnetic order in the PFW‐BFO solid solution are discussed from the point view of the variations in both the –Fe–O–Fe– and –Fe–O–W–O–Fe– superexchange routes, which are intimately related to the ratio of magnetic Fe 3+ ion concentration on the B‐site and the changes in the local structural order/disorder and chemical homogeneities. Combining the magnetic phase diagram with the relaxor characteristic phase diagram of the (1‐ x )PFW‐ x BFO system, a striking feature is found that the ergodic relaxor (ER) state and the weakly ferromagnetic phase coexist in the composition range of 0.025 ≤ x ≤ 0.1 between the freezing temperature T f and the Burns temperature T B . Abstract : The combined magnetic and relaxor phase diagram established for the multiferroic (1‐x)Pb(Fe2/3 W1/3 )O3 ‐xBiFeO3 solid solution, showing that the ergotic relaxor (ER) state and the weakly ferromagnetic (WFM2 ) phase coexist in the composition range of 0.025 ≤ x ≤ 0.1 between the freezing temperature Tf and the Burns temperature TB . It is expected that the coupling between the weakly ferromagnetic order with magnetic clusters and the ergotic relaxor (ER) state with differently correlated polar clusters could enhance magnetoelectric coupling effect and lead to some new kinds of magnetoelectric effects in PFW‐BFO. ​