Abstract

Magnetic ordering could have significant influence on band structures, spin-dependent transport, and other important properties of materials. Its measurement, especially for the case of antiferromagnetic (AFM) ordering, however, is generally difficult to be achieved. Here we demonstrate the feasibility of magnetic ordering detection using a noncontact and nondestructive optical method. Taking the tetragonal BiFeO3 (BFO) as an example and combining density functional theory calculations with tight-binding models, we find that when BFO changes from C1-type to G-type AFM phase, the top of valance band shifts from the Z point to Γ point, which makes the original direct band gap become indirect. This can be explained by Slater-Koster parameters using the Harrison approach. The impact of magnetic ordering on band dispersion dramatically changes the optical properties. For the linear ones, the energy shift of the optical band gap could be as large as 0.4 eV. As for the nonlinear ones, the change is even larger. The second-harmonic generation coefficient d33 of G-AFM becomes more than 13 times smaller than that of C1-AFM case. Finally, we propose a practical way to distinguish the two AFM phases of BFO using the optical method, which is of great importance in next-generation information storage technologies.

Highlights

  • In tetragonal phase with giant c/a ratio and find sizable differences for both linear and nonlinear optical properties between C1- and G-antiferromagnetic (AFM) ordering

  • There exists a transition between C1- and G-type AFM ordering for tetragonal BFO under the influence of in-plane strain[19,52]

  • Using first-principles calculations, we found that the different spin arrangements in tetragonal BFO have significant influence on the dispersion of energy bands, especially the location of the highest occupied molecular orbital (HOMO), which has been explained by the minimal one-band TB models

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Summary

Introduction

In tetragonal phase with giant c/a ratio and find sizable differences for both linear and nonlinear optical properties between C1- and G-antiferromagnetic (AFM) ordering. The predicted modification of optical properties induced by magnetic ordering change reveals the possibility of using a noncontact and nondestructive optical method to distinguish the C1- and G-type AFM of BFO, which is currently hard to be handled by a traditional neutron diffraction measurement because of the strong diamagnetic response of substrate materials[50]

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