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Magnetic Weyl semimetals with diamond structure realized in spinel compounds

MetadataDetails
Publication Date2020-03-18
JournalPhysical review. B./Physical review. B
AuthorsWei Jiang, Huaqing Huang, Feng Liu, Jian‐Ping Wang, Tony Low
InstitutionsUniversity of Utah, University of Minnesota
Citations29
AnalysisFull AI Review Included

Technical Documentation: Magnetic Weyl Semimetals in Diamond-Structure Spinels

Section titled “Technical Documentation: Magnetic Weyl Semimetals in Diamond-Structure Spinels”

This document analyzes the research on realizing Magnetic Weyl Semimetals (WSMs) within a diamond lattice structure, specifically in VMg2O4 spinel compounds. The findings are highly relevant to engineers and scientists utilizing high-purity CVD diamond platforms for advanced spintronics and quantum material research.


The research introduces a novel $e_g$-orbital diamond model that hosts complex topological states, demonstrating its realization in spinel compounds, which share the Fd-3m space group symmetry with diamond.

  • Topological Discovery: Identification of a 3D Nodal Cage (NC) feature and hourglass fermions protected by orbital and sublattice degeneracies within the $e_g$-diamond model.
  • Material Realization: The model is realized in the 4-2 spinel VMg2O4, where the A-site cations form a perfect diamond sublattice structure.
  • Half-Metallicity: VMg2O4 exhibits ideal half-metallicity, crucial for spintronics, characterized by one metallic spin channel and one insulating channel with a large spin gap (up to 6.62 eV).
  • Magnetic Weyl Semimetal: Inclusion of Spin-Orbit Coupling (SOC) transforms the system into a Magnetic Weyl Semimetal (WSM) state, confirmed by 18 pairs of Weyl points and topological Fermi arcs.
  • Integration Potential: VMg2O4 shows excellent lattice matching (< 0.4% mismatch) with MgO, facilitating integration into industrial spintronics devices (e.g., Magnetic Tunneling Junctions, MTJs).
  • Application Focus: The findings open pathways for developing low switching energy magnetic devices and utilizing the unique properties of diamond-structure topological materials.

The following hard data points were extracted from the first-principles calculations on VMg2O4:

ParameterValueUnitContext
Spin Gap (PBE Level)4.36eVHalf-metallicity feature (Spin Down Channel)
Spin Gap (HSE Level)6.62eVEnhanced gap using Hybrid Functionals
Magnetic Moment2”B per UCFerromagnetic (FM) state, primarily contributed by V cations
FM/AFM Energy Difference0.43eVIndicates promising room temperature FM stability
Nodal Point Proximity< 20meVEnergy dispersion of nodal points relative to the Fermi level
Lattice Mismatch with MgO< 0.4%Critical for epitaxial growth on (001) and (111) planes
Anomalous Hall Conductivity (Peak)≈ 100Ω-1 cm-1Intrinsic anomalous Hall conductivity (σHA)
Crystal StructureFd-3mSpace GroupSame symmetry as the diamond lattice

The research utilized advanced computational techniques to model and confirm the topological states derived from the $e_g$-diamond structure:

  1. Tight-Binding (TB) Model Development: A novel 3D $e_g$-orbital diamond model was constructed, incorporating both nearest-neighbor (NN) and next-nearest-neighbor (NNN) hopping interactions to analyze band structure and degeneracy.
  2. First-Principles DFT Calculations: Density Functional Theory (DFT) calculations were performed on the 4-2 spinel VMg2O4 to determine electronic and magnetic ground states (Ferromagnetic).
  3. Half-Metallicity Confirmation: Band structures were calculated without Spin-Orbit Coupling (SOC) to confirm the ideal half-metallic state and the large spin gap in the insulating channel.
  4. Wannier Function Fitting: Maximally Localized Wannier Functions (MLWFs) were used to accurately fit the DFT band structures, confirming the orbital characteristics ($d_{z^2}$ and $d_{x^2-y^2}$) consistent with the $e_g$-diamond model.
  5. Topological State Analysis: 3D band structures and 2D k-plane cuts were analyzed to confirm the formation of the 3D Nodal Cage (NC) feature near the Fermi level.
  6. Magnetic Weyl Semimetal Confirmation: Non-collinear calculations including SOC were performed, demonstrating the breaking of degeneracy and the transition to a Magnetic Weyl Semimetal state characterized by 18 pairs of Weyl points.
  7. Surface State and Transport Calculation: Topological surface states, Fermi arcs, and intrinsic anomalous Hall conductivity (σHA) were calculated using Green’s function methods to verify the WSM phase.

The realization of complex topological states based on the diamond lattice structure presents a unique opportunity for 6CCVD to supply high-purity CVD diamond materials as foundational platforms for next-generation spintronics research.

The research relies on the structural perfection inherent in the diamond lattice. 6CCVD provides materials that serve as ideal templates, substrates, or functional components for replicating and extending this work:

  • Optical Grade Single Crystal Diamond (SCD): Required for applications demanding the highest structural integrity and lowest defect density. SCD provides a perfect crystalline platform (Ra < 1 nm polishing) necessary for studying subtle topological effects and integrating high-quality epitaxial films like VMg2O4.
  • Boron-Doped Diamond (BDD): Ideal for use as robust, conductive electrodes or substrates in transport experiments (e.g., measuring the anomalous Hall conductivity, σHA). BDD offers tunable conductivity without compromising chemical inertness.

The proposed application involves complex stacking (e.g., VMg2O4/MgO/VMg2O4 MTJs). 6CCVD’s custom manufacturing capabilities directly address the needs of device fabrication:

Research Requirement6CCVD CapabilityTechnical Specification
Custom Substrate DimensionsCustom plates and wafers up to 125 mm in diameter (PCD) or large-area SCD.Plates/wafers up to 125 mm (PCD). Substrates up to 10 mm thick.
Precise Film ThicknessSCD and PCD materials available in ultra-thin film formats.Thickness range: 0.1 ”m to 500 ”m (SCD/PCD).
Electrical Contact IntegrationIn-house metalization services for electrode deposition.Custom metal stacks including Au, Pt, Pd, Ti, W, and Cu.
Surface QualityUltra-low roughness polishing essential for epitaxial growth.Polishing: Ra < 1 nm (SCD), Ra < 5 nm (Inch-size PCD).

The theoretical discovery of the $e_g$-diamond model and its realization in VMg2O4 requires specialized material knowledge for experimental validation.

  • Material Selection for Spintronics: 6CCVD’s in-house PhD team can assist researchers in selecting the optimal diamond material (SCD vs. PCD vs. BDD) and surface orientation required for the epitaxial growth of spinel compounds and subsequent measurement of topological properties (e.g., Fermi arcs and anomalous Hall effect).
  • Interface Optimization: We provide consultation on surface preparation and metalization schemes necessary to create low-resistance contacts for high-frequency or quantum transport measurements in these novel magnetic Weyl semimetal systems.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.

View Original Abstract

Diamond-structure materials have been extensively studied for decades, which\nform the foundation for most semiconductors and their modern day electronic\ndevices. Here, we discover a e$g$-orbital ($d{z^2}$,$d_{x^2-y^2}$ ) model\nwithin the diamond lattice (e$_g$-diamond model) that hosts novel topological\nstates. Specifically, the e$_g$-diamond model yields a 3D nodal cage (3D-NC),\nwhich is characterized by a $d$-$d$ band inversion protected by two types of\ndegenerate states (i.e., e$_g$-orbital and diamond-sublattice degeneracies). We\ndemonstrate materials realization of this model in the well-known spinel\ncompounds (AB$_2$X$_4$), where the tetrahedron-site cations (A) form the\ndiamond sub-lattice. An ideal half metal with one metallic spin channel formed\nby well-isolated and half-filled e$_g$-diamond bands, accompanied by a large\nspin gap (4.36 eV) is discovered in one 4-2 spinel compound (VMg$_2$O$_4$),\nwhich becomes a magnetic Weyl semimetal when spin-orbit coupling effect is\nfurther considered. Our discovery greatly enriches the physics of diamond\nstructure and spinel compounds, opening a door to their application in\nspintronics.\n