Fig. 5: Temporal non-Abelian AB interference in a three-dimensional gauge field.

Theoretical calculation results of the intensity contrast a–c ρ12 and d–f ρ13 between the degenerate states after the non-Abelian interference versus parameters initial intensity distribution α, β and phase differences ξ for χ = 0, π/2, and π, respectively. Numerical simulation results of the intensity contrast g–i ρ12 and j–l ρ13 versus parameters α, β and ξ for χ = 0, π/2, and π, respectively.