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Manipulating Spin–Lattice Coupling in Layered Magnetic Topological Insulator Heterostructure via Interface Engineering

Abstract Induced magnetic order in a topological insulator (TI) can be realized either by depositing magnetic adatoms on the surface of a TI or engineering the interface with epitaxial thin film or stacked assembly of 2D van der Waals (vdW) materials. Herein, the observation of spin‐phonon coupling...

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Published in:Advanced functional materials 2024-05, Vol.34 (38)
Main Authors: Maity, Sujan, Dey, Dibyendu, Ghosh, Anudeepa, Masanta, Suvadip, De, Binoy Krishna, Kunwar, Hemant Singh, Das, Bikash, Kundu, Tanima, Palit, Mainak, Bera, Satyabrata, Dolui, Kapildeb, Watanabe, Kenji, Taniguchi, Takashi, Yu, Liping, Taraphder, A., Datta, Subhadeep
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container_issue 38
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container_title Advanced functional materials
container_volume 34
creator Maity, Sujan
Dey, Dibyendu
Ghosh, Anudeepa
Masanta, Suvadip
De, Binoy Krishna
Kunwar, Hemant Singh
Das, Bikash
Kundu, Tanima
Palit, Mainak
Bera, Satyabrata
Dolui, Kapildeb
Watanabe, Kenji
Taniguchi, Takashi
Yu, Liping
Taraphder, A.
Datta, Subhadeep
description Abstract Induced magnetic order in a topological insulator (TI) can be realized either by depositing magnetic adatoms on the surface of a TI or engineering the interface with epitaxial thin film or stacked assembly of 2D van der Waals (vdW) materials. Herein, the observation of spin‐phonon coupling in the otherwise non‐magnetic TI Bi 2 Te 3 is reported, due to the proximity of FePS 3 (an antiferromagnet (AFM), T N ≈ 120 K), in a vdW heterostructure framework. Temperature‐dependent Raman spectroscopic studies reveal deviation from the usual phonon anharmonicity originated from spin‐lattice coupling at the Bi 2 Te 3 /FePS 3 interface at/below 60 K in the peak position (self‐energy) and linewidth (lifetime) of the characteristic phonon modes of Bi 2 Te 3 (106 and 138 cm −1 ) in the stacked heterostructure. The Ginzburg‐Landau (GL) formalism, where the respective phonon frequencies of Bi 2 Te 3 couple to phonons of similar frequencies of FePS 3 in the AFM phase, is adopted to understand the origin of the hybrid magneto‐elastic modes. At the same time, the reduction of characteristic T N of FePS 3 from 120 K in isolated flakes to 65 K in the heterostructure, possibly due to the interfacial strain, which leads to smaller Fe‐S‐Fe bond angles as corroborated by computational studies using density functional theory (DFT). Besides, inserting hexagonal boron nitride within Bi 2 Te 3 /FePS 3 stacking regains the anharmonicity in Bi 2 Te 3 . Controlling interfacial spin‐phonon coupling in stacked heterostructure can have potential application in surface code spin logic devices.
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At the same time, the reduction of characteristic T N of FePS 3 from 120 K in isolated flakes to 65 K in the heterostructure, possibly due to the interfacial strain, which leads to smaller Fe‐S‐Fe bond angles as corroborated by computational studies using density functional theory (DFT). Besides, inserting hexagonal boron nitride within Bi 2 Te 3 /FePS 3 stacking regains the anharmonicity in Bi 2 Te 3 . 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title Manipulating Spin–Lattice Coupling in Layered Magnetic Topological Insulator Heterostructure via Interface Engineering
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