Abstract

We investigated the relative importance of removing the Mn3+ Jahn-Teller distortion in driving ferromagnetism in LaMn1-xScxO3 combining x-ray powder diffraction and x-ray absorption spectroscopy at the Mn and Sc K-edges. By increasing the Sc content, the orthorhombic distortion of the Pbnm cell in LaMnO3 decreases but the unit-cell remains slightly distorted in LaScO3. Besides, the nearly tetragonal-distorted MO6 in LaMnO3 continuously evolves into a nearly regular one in LaScO3. On the other hand, x-ray absorption spectra show that the MnO6 octahedron remains Jahn-Teller distorted and the ScO6 octahedron is nearly regular along the whole series. Moreover, the ordering of the Mn3+ Jahn-Teller distortion is not disrupted in the ab plane for any Sc concentration. This contrasts with the Ga- substituted compounds, where a regular MnO6 is found for x>0.5. However, both LaMn0.5Sc0.5O3 and LaMn0.5Ga0.5O3 show ferromagnetic behavior independently of the presence (or not) of Jahn-Teller distorted Mn3+. Thus, our results point to the Mn-sublattice dilution as the main effect in driving ferromagnetism in these manganites over local structure effects previously proposed by the spin flipping or the vibronic superexchange models.

Highlights

  • Doped manganites have been extensively studied owing to their colossal magnetoresistance property and its potential applications to magnetic devices

  • It is known that the A-type AFM orbitally ordered state of LaMnO3 is easy destroyed to give way to ferromagnetism (FM) by introducing various cations on the Mn site [2,3,4,5]

  • We have studied the crystallographic structure by x-ray powder diffraction (XRD) and the local structure by x-ray absorption spectroscopy (XAS) at the Mn and Sc K-edges in the LaMn1-xScxO3 series in order to clarify the importance of removing the Jahn-Teller distortion in driving the FM behavior

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Summary

Introduction

Doped manganites have been extensively studied owing to their colossal magnetoresistance property and its potential applications to magnetic devices. Both models assume that the change from A-type AFM to FM ordering is originated by the orbital direction adopted by the Mn3+ ion and it is similar for Ga and Sc non-magnetic substitutions, so the atomic eg orbital would be perturbed in the same way for the two series.

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