Quantum geometry quadrupole-induced third-order nonlinear transport in antiferromagnetic topological insulator MnBi₂Te₄.

Abstract

The study of quantum geometry effects in materials has been one of the most important research directions in recent decades. The quantum geometry of a material is characterized by the quantum geometric tensor of the Bloch states. The imaginary part of the quantum geometry tensor gives rise to the Berry curvature while the real part gives rise to the quantum metric. While Berry curvature has been well studied in the past decades, the experimental investigation on the quantum metric effects is only at its infancy stage. In this work, we measure the nonlinear transport of bulk MnBi₂Te₄, which is a topological anti-ferromagnet_. We found that the second order nonlinear responses are negligible as required by inversion symmetry, the third-order nonlinear responses are finite. The measured third-harmonic longitudinal ( <math xmlns="http://www.w3.org/1998/Math/MathML"> <msubsup><mrow><mi>V</mi></mrow> <mrow><mi>x</mi> <mi>x</mi></mrow> <mrow><mn>3</mn> <mi>ω</mi></mrow> </msubsup> </math> ) and transverse ( <math xmlns="http://www.w3.org/1998/Math/MathML"> <msubsup><mrow><mi>V</mi></mrow> <mrow><mi>x</mi> <mi>y</mi></mrow> <mrow><mn>3</mn> <mi>ω</mi></mrow> </msubsup> </math> ) voltages with frequency 3 <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ω</mi></math> , driven by an a.c. current with frequency <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>ω</mi></math> , show an intimate connection with magnetic transitions of MnBi₂Te₄ flakes. Their magnitudes change abruptly as MnBi₂Te₄ flakes go through magnetic transitions from an antiferromagnetic state to a canted antiferromagnetic state and to a ferromagnetic state. In addition, the measured <math xmlns="http://www.w3.org/1998/Math/MathML"> <msubsup><mrow><mi>V</mi></mrow> <mrow><mi>x</mi> <mi>x</mi></mrow> <mrow><mn>3</mn> <mi>ω</mi></mrow> </msubsup> </math> is an even function of the applied magnetic field B while <math xmlns="http://www.w3.org/1998/Math/MathML"> <msubsup><mrow><mi>V</mi></mrow> <mrow><mi>x</mi> <mi>y</mi></mrow> <mrow><mn>3</mn> <mi>ω</mi></mrow> </msubsup> </math> is odd in B. Amazingly, the field dependence of the third-order responses as a function of the magnetic field suggests that <math xmlns="http://www.w3.org/1998/Math/MathML"> <msubsup><mrow><mi>V</mi></mrow> <mrow><mi>x</mi> <mi>x</mi></mrow> <mrow><mn>3</mn> <mi>ω</mi></mrow> </msubsup> </math> is induced by the quantum metric quadrupole and <math xmlns="http://www.w3.org/1998/Math/MathML"> <msubsup><mrow><mi>V</mi></mrow> <mrow><mi>x</mi> <mi>y</mi></mrow> <mrow><mn>3</mn> <mi>ω</mi></mrow> </msubsup> </math> is induced by the Berry curvature quadrupole. Therefore, the quadrupoles of both the real and the imaginary part of the quantum geometry tensor of bulk MnBi₂Te₄ are revealed through the third order nonlinear transport measurements. This work greatly advanced our understanding on the connections between the higher order moments of quantum geometry and nonlinear transport.