“…These transitions create three Λ-systems consisting of (σ + , π), (σ − , π), and (σ + , σ − ) light components. So, the formation of these Λ-systems allows optical coupling among different ground state Zeeman sublevels (m g = 0, ±1) via an excited state Zeeman sublevel (m e = 0) [19,28]. This coupling of ground state sublevels creates the Hanle resonance as the function of the magnetic field B s .…”