Rubidium-87 clock transition ($|1,0⟩\leftrightarrow |2,0⟩$)

The ground-hyperfine magnetic-dipole transition between $F=1,m_F=0$ and $F=2,m_F=0$ has vanishing first-order Zeeman shift near zero field. It obeys $\Delta F=1,\Delta m_F=0$. Its residual quadratic shift follows from the Breit-Rabi formula, rather than from assigning both states permanently zero magnetic dipole moment.