# High-temperature ferroelectric order and magnetic field-cooled effect driven magnetoelectric coupling in R2BaCuO5 (R= Er, Dy, Sm)

## TL;DR

This study reports high-temperature ferroelectric order and a unique magnetoelectric effect driven by magnetic field cooling in R2BaCuO5 (R=Er, Dy, Sm), with promising polarization values and structural insights.

## Contribution

It reveals high-temperature ferroelectricity and a novel magnetoelectric coupling mechanism in R2BaCuO5 compounds, expanding understanding of multiferroic materials.

## Key findings

- Ferroelectric order observed above 230 K with high polarization.
- Unusual magnetoelectric coupling occurs below magnetic ordering temperatures.
- Magnetoelectric effect driven by magnetic field cooling is reversible with poling field.

## Abstract

The high-temperature ferroelectric order and a remarkable magnetoelectric effect driven by the magnetic field cooling are reported in R2BaCuO5 (R = Er, Dy, Sm) series. The ferroelectric (FE) orders are observed at much higher temperatures than their magnetic orders for all three members. The value of FE Curie temperature (TFE) is considerably high as ~ 235 K with the polarization value (P) of ~ 1410 {\mu}C/m2 for a 4 kV/cm poling field in case of Er2BaCuO5, whereas the values of TFE and P are also promising as ~ 232 K and ~ 992 {\mu}C/m2 for Dy2BaCuO5, and ~ 184 K and ~ 980 {\mu}C/m2 for Sm2BaCuO5. The synchrotron diffraction studies of Dy2BaCuO5 confirm a structural transition at TFE to a polar Pna21 structure, which correlates the FE order. An unusual magnetoelectric coupling is observed below the R order for Er and Dy compounds and below the Cu order for Sm compound, when the pyroelectric current is recorded only with the magnetic field both in heating and cooling cycles i.e. typical magnetic field cooled effect. The magnetic field cooled effect driven emergence of polarization is ferroelectric in nature, as it reverses due to the opposite poling field. The unexplored R2BaCuO5 series attracts the community for large TFE, high P value, and strange magnetoelectric consequences.