WEYL SEMIMETAL

Topological band crossing · Chiral anomaly

OBSERVABLES

Chern number (each node)±1
∂_μ j^μ_5 (anomaly)
LMR (neg. mag. resist.)
Fermi arc length
∂_t ρ_χ = χ e²/(4π²ℏ) E·B
Weyl nodes are monopoles of Berry curvature in k-space. Parallel E and B pump chirality (ABJ anomaly): right-handed node fills, left empties. This gives negative longitudinal magnetoresistance — the experimental signature of Weyl semimetals (TaAs, NbP, WTe₂).