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Giant tunneling magnetoresistance and electroresistance in a two-dimensional <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>VSi</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi mathvariant="normal">N</mml:mi> <mml:mn>4</mml:mn> </mml:msub> </mml:mrow> </mml:math> / <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>In</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi>Te</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:mrow> </mml:math> multiferroic tunnel junction

Shili Yang, Zhifan Zheng, Hua Hao, Chun-Sheng Liu, Xiaohong Zheng, Lei Zhang

2024Physical review. B./Physical review. B12 citationsDOI

Abstract

${\mathrm{VSi}}_{2}{\mathrm{N}}_{4}$ is a newly reported magnetic semiconductor and is promising for being turned into a half metal. For this purpose, we construct a ${\mathrm{VSi}}_{2}{\mathrm{N}}_{4}$/${\mathrm{In}}_{2}{\mathrm{Te}}_{3}$ van der Waals multiferroic heterostructure based on first-principles calculations. It is found that the inversion of ferroelectric polarization of monolayer ${\mathrm{In}}_{2}{\mathrm{Te}}_{3}$ can efficiently modulate the electronic states of monolayer ${\mathrm{VSi}}_{2}{\mathrm{N}}_{4}$. A phase transition of ${\mathrm{VSi}}_{2}{\mathrm{N}}_{4}$ from semiconductor to half metal can be effectually realized, leading to distinct electronic transport properties. Next, we design a magnetic tunnel junction (MTJ) (using the ${\mathrm{VSi}}_{2}{\mathrm{N}}_{4}$ monolayer as the tunneling barrier and the multiferroic heterostructure as the electrode) and investigate its transport properties in various magnetic configurations under different polarization directions of the ferroelectric ${\mathrm{In}}_{2}{\mathrm{Te}}_{3}$ layer by combining the nonequilibrium Green's function with density functional theory. The results show that the junction exhibits half-metallic transport in the parallel magnetic configuration and near-zero transport in the antiparallel magnetic configuration, resulting in a giant tunneling magnetoresistance ratio of $\ensuremath{\sim}1\ifmmode\times\else\texttimes\fi{}{10}^{12}%$. Moreover, a $\ensuremath{\sim}1\ifmmode\times\else\texttimes\fi{}{10}^{17}%$ tunneling electroresistance ratio is achieved in the parallel magnetic configuration accompanying the polarization reversal. The findings suggest that MTJs based on the ${\mathrm{VSi}}_{2}{\mathrm{N}}_{4}$/${\mathrm{In}}_{2}{\mathrm{Te}}_{3}$ heterojunction have great potential for applications in multifunctional spintronic devices.

Topics & Concepts

Quantum tunnellingMaterials scienceComputer sciencePhysicsCondensed matter physics2D Materials and ApplicationsGraphene research and applicationsQuantum Dots Synthesis And Properties
Giant tunneling magnetoresistance and electroresistance in a two-dimensional <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>VSi</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi mathvariant="normal">N</mml:mi> <mml:mn>4</mml:mn> </mml:msub> </mml:mrow> </mml:math> / <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>In</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi>Te</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:mrow> </mml:math> multiferroic tunnel junction | Litcius