Magnetism-induced second-order nonlinear optical responses in multiferroic BiFeO$_3$

TL;DR

This study extends the calculation of second-order nonlinear optical responses to magnetic multiferroic BiFeO3, revealing large, tunable magnetism-induced effects useful for spintronics and photovoltaic applications.

Contribution

The paper introduces a modified formula for magnetic systems to calculate magnetism-induced NLO responses, specifically in BiFeO3, demonstrating significant, controllable effects.

Findings

Large magnetism-induced SHG susceptibilities in BiFeO3

SHG intensity is tunable with magnetization reversal

Strong BPVE responses surpassing some well-known NLO materials

Abstract

Nonlinear optical (NLO) responses of noncentrosymmetric nonmagnets have drawn a lot of attention in the past decades because of their significance in materials characterization, green energy and device applications. However, the magnetism-induced NLO responses have rarely been studied so far. In this paper, we first extend the numerical calculation friendly formula by Rashkeev $\textit{et al.}$ [Phys. Rev. B $\textbf{57}$, 3905 (1998)] for second harmonic generation (SHG) in nonmagnetic materials to include magnetic systems and then calculate the magnetism-induced NLO responses of BiFeO$_3$, a multiferroic that exhibits both ferroelectricity and antiferromagnetic (AFM) ordering at room temperature and has a band gap that falls in the visible frequency region. First, we find that the calculated magnetism-induced SHG susceptibilities are large and the SHG intensity is tunable with the reversal of magnetization. In particular, we find a strong magnetic contrast of the SHG signal of approximately 440% at SHG photon energy of 4.82 eV, thus enabling a magnetic control of the SHG in BiFeO$_3$. Also, because of the sensitivity of the SHG signal to the direction of the N\'eel vector, the SHG can be utilized to detect the reversal of the N\'eel vector in the AFM materials, which is an important issue for AFM spintronics. Second, the calculated BPVE in BiFeO$_3$ are also strong, being larger than some well-known NLO compounds such as BaTiO$_3$, GaAs, CdS and CdSe. Finally, we analyse the origins of the prominent features in the NLO response spectra in terms of the calculated quantum geometric quantities. Our interesting findings suggest that the magnetism-driven NLO responses in BiFeO$_3$ are significant, anisotropic and tunable, and that understanding the magnetism-driven components of both SHG and BPVE is essential for their applications in, e.g., multiferroic-based photovoltaic devices.