Research··5 min read

Four double-Weyl fermions and their topological phase transitions in nonmagnetic crystals

The work derives crystalline constraints for exactly four symmetry-protected double-Weyl points, proposes THRLN-C32, and reveals several strain-driven topological transition pathways.

Fig. 2 | Bulk bands, orbital-resolved density of states, Berry phases and double-Weyl dispersions for left- and right-handed THRLN-C32.
Fig. 2 | Bulk bands, orbital-resolved density of states, Berry phases and double-Weyl dispersions for left- and right-handed THRLN-C32. · Figure source · CC BY 4.0

The minimal four-double-Weyl problem

Nonmagnetic crystals require at least four conventional Weyl points, yet the symmetry conditions and material realization for exactly four charge-two double-Weyl points had remained unresolved.

Strict crystalline-symmetry constraints

A systematic analysis of nonmagnetic spinless and spinful systems shows that exactly four symmetry-protected double-Weyl points are restricted to only twenty-eight space groups, sharply narrowing the material search space.

The THRLN-C32 platform

The symmetry screening identifies the sp2–sp3-hybridized chiral carbon allotrope THRLN-C32. First-principles calculations place four C4-protected double-Weyl points near the Fermi level, with extended or closed-loop Fermi arcs on the surface.

A strain-driven transition landscape

Applied strain can transform the four-double-Weyl phase into two three-terminal Weyl complexes, eight conventional Weyl points, or a fully gapped trivial insulator, yielding a unified transition landscape.

Why it matters

The study establishes the symmetry boundary and a candidate material for nonmagnetic double-Weyl semimetals while showing how strain can control complex topological node structures.

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