Intralayer strain tuned interlayer magnetism in bilayer CrSBr

Intralayer strain tuned interlayer magnetism in bilayer CrSBr

Nanshu Liu, Cong Wang, Changlin Yan, Changsong Xu, Jun Hu, Yanning Zhang, and Wei Ji

Interlayer magnetism was tuned by many interlayer means, e.g., stacking, distance, and external fields in
two-dimensional (2D) magnets. As an exception, the interlayer magnetism of CrSBr few layers was, however,
experimentally changed by applied intralayer strains [Nat. Nanotechnol. 17, 256 (2022)], the mechanism of
which is yet to be unveiled. Here, we uncovered its mechanism by investigating in-plane strained bilayer
CrSBr using density functional theory calculations. Under in-plane tensile strain, wavefunction overlaps are
strengthened for Br p electrons within each CrSBr layer, which delocalizes intralayer electrons and, as a
consequence, promotes interlayer electron hopping. A negative interlayer Poisson’s ratio also enlarges interlayer
spacing for bilayer CrSBr, which reduces the interlayer Pauli repulsion. This joint effect, further verified by
examining interlayer sliding and interfacial element substitution, leads to an interlayer antiferromagnetic to
ferromagnetic transition, consistent with the previous experimental observation. This mechanism enables a route
to tune interlayer magnetism by modifying intralayer electron localization in 2D magnets.

Competing multiferroic phases in monolayer and few-layer NiI2

Competing multiferroic phases in monolayer and few-layer NiI2

Nanshu Liu, Cong Wang, Changlin Yan, Changsong Xu, Jun Hu, Yanning Zhang, and Wei Ji

A recent experiment reported type-II multiferroicity in monolayer (ML) NiI2 based on a presumed spiral magnetic configuration (Spiral-B), which is, as we found here, under debate in the ML limit. Freestanding ML NiI2 breaks its C3 symmetry, as it prefers a striped antiferromagnetic order (AABB-AFM) along with an intralayer antiferroelectric (AFE) order. However, substrate confinement may preserve the C3 symmetry and/or apply tensile strain to the ML. This leads to another spiral magnetic order (SpiralIVX), while 2L shows a different order (SpiralVX) and Spiral-B dominates in thicker layers. Thus, three multiferroic phases, namely, SpiralB+FE, Spiral-IVX +FE, Spiral-VX+FE, and an anti-multiferroic AABB-AFM+AFE one, show layer-thickness-dependent and geometry-dependent dominance, ascribed to competitions among thickness-dependent Kitaev, biquadratic, and Heisenberg spin–exchange interactions and single-ion magnetic anisotropy. Our theoretical results clarify the debate on the multiferroicity of ML NiI2 and shed light on the role of layer-stacking-induced changes in noncollinear spin–exchange interactions and magnetic anisotropy in thickness-dependent magnetism.

Spin-resolved imaging of atomic-scale helimagnetism in mono- and bi-layer NiI2

Spin-resolved imaging of atomic-scale helimagnetism in mono- and bi-layer NiI2

Mao-Peng Miao, Nanshu Liu, Wen-Hao Zhang, Jian-Wang Zhou, Dao-Bo Wang, Cong Wang, Wei Ji, and Ying-Shuang Fu

Noncollinear magnetic orders in monolayer van der Waals magnets are crucial for probing delicate magnetic interactions under minimal spatial constraints and advancing miniaturized spintronic devices. Despite their significance, achieving atomic-scale identification remains challenging. In this study, we utilized spin-polarized scanning tunneling microscopy and density functional theory calculations to identify spin-spiral orders in mono- and bi-layer NiI2, grown on graphene-covered SiC(0001) substrates. We discovered two distinct spin-spiral states with Q vectors aligning and deviating by 7° from the lattice direction, exhibiting periodicities of 4.54 and 5.01 times the lattice constant, respectively. These findings contrast with bulk properties and align closely with our theoretical predictions. Surprisingly, the finite sizes of monolayers induce incommensurability with the spin-spiral period, facilitating collective spin switching behavior under magnetic fields. Our research reveals intrinsic noncollinear magnetism at the monolayer limit with unprecedented resolution, paving the way for exploring novel spin phenomena.

Atomically engineering metal vacancies in monolayer transition metal dichalcogenides

Atomically engineering metal vacancies in monolayer transition metal dichalcogenides

Nature Synthesis 3, 586–594 (2024).

Xiaocang Han, Mengmeng Niu, Yan Luo, Runlai Li, Jiadong Dan, Yanhui Hong, Xu Wu, Alex V. Trukhanov, Wei Ji, Yeliang Wang, Jiahuan Zhou, Jingsi Qiao*, Jin Zhang* & Xiaoxu Zhao*

Abstract:

Scanning probe microscopy and scanning transmission electron microscopy (STEM) are powerful tools to trigger atomic-scale motions, pattern atomic defects and lead to anomalous quantum phenomena in functional materials. However, these techniques have primarily manipulated surface atoms or atoms located at the beam exit plane, leaving buried atoms, which govern exotic quantum phenomena, largely unaffected. Here we propose an electron-beam-triggered chemical etching approach to engineer shielded metal atoms sandwiched between chalcogen layers in monolayer transition metal dichalcogenide (TMDC). Various metal vacancies (V_MX_n, n=0−6) have been fabricated via atomically focused electron beam in STEM. The parent TMDC surface was modified with surfactants, facilitating the ejection of sandwiched metal vacancies via charge transfer effect. In situ sequential STEM imaging corroborated that a combined chemical-induced knock-on effect and chalcogen vacancy-assisted metal diffusion process result in atom-by-atom vacancy formation. This approach is validated in 16 different TMDCs. The presence of metal vacancies strongly modified their magnetic and electronic properties, correlated with the unpaired chalcogen p and metal d electrons surrounding vacancies and adjacent distortions. These findings show a generic approach for engineering interior metal atoms with atomic precision, creating opportunities to exploit quantum phenomena at the atomic scale.

DOI:10.1038/s44160-024-00501-z

TOC Figure

Conversion of chirality to twisting via sequential one-dimensional and two-dimensional growth of graphene spirals

Conversion of chirality to twisting via sequential one-dimensional and two-dimensional growth of graphene spirals

Nature Materials 23, 331–338 (2024).

Zhu-Jun Wang#,*, Xiao Kong#, Yuan Huang#, Jun Li#, Lihong Bao, Kecheng Cao, Yuxiong Hu, Jun Cai, Lifen Wang, Hui Chen, Yueshen Wu, Yiwen Zhang, Fei Pang, Zhihai Cheng, Petr Babor, Miroslav Kolibal, Zhongkai Liu, Yulin Chen, Qiang Zhang, Yi Cui, Kaihui Liu, Haitao Yang, Xinhe Bao, Hong-Jun Gao, Zhi Liu, Wei Ji*, Feng Ding* & Marc-Georg Willinger*

Abstract:

The properties of two-dimensional (2D) van der Waals materials can be tuned through nanostructuring or controlled layer stacking, where interlayer hybridization induces exotic electronic states and transport phenomena. Here we describe a viable approach and underlying mechanism for the assisted self-assembly of twisted layer graphene. The process, which can be implemented in standard chemical vapour deposition growth, is best described by analogy to origami and kirigami with paper. It involves the controlled induction of wrinkle formation in single-layer graphene with subsequent wrinkle folding, tearing and re-growth. Inherent to the process is the formation of intertwined graphene spirals and conversion of the chiral angle of 1D wrinkles into a 2D twist angle of a 3D superlattice. The approach can be extended to other foldable 2D materials and facilitates the production of miniaturized electronic components, including capacitors, resistors, inductors and superconductors.

DOI: 10.1038/s41563-023-01632-y

Also See: News & Views – A double-helix dislocation in graphene | Nature Materials
Also See: Focus – Constructing 2D moiré and chiral materials | Nature Materials