Abstract

Ferroelectric and magnetic properties of Fe1−xMnxV2O4 (0 ≤ x ≤ 0.5) spinels are investigated on the basis of dielectric, polarization, and susceptibility measurements. Ferroelectric polarization is discovered in collinear ferrimagnetic and Yafet–Kittel magnetic phases for 0.1 ≤ x ≤ 0.4, which can be tuned by a magnetic field. As orbital-active Fe2+ is substituted with Mn2+, ferroelectric polarization decreases for 0 ≤ x ≤ 0.4 and disappears for x = 0.5. We propose that the two polar components in ferroelectric polarization originate from the exchange striction mechanism and the spin-current model, respectively.

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