3D Dirac Semimetal — Linear Band Crossing

Bulk Dirac Cones · Surface States · Bulk-Boundary Correspondence


Parameters

H(k) = vF(k·σ) + mσz
E±(k) = ±√(vF²|k|² + m²)
Dirac point: m=0, |k|=0
Two Dirac nodes at ±kD on kz-axis
A 3D Dirac semimetal hosts 4-fold degenerate band crossings protected by crystal symmetry. Each Dirac point splits into two Weyl nodes upon breaking inversion or time-reversal symmetry.