“…From the dressed-state theory, the excited state |2 is dressed by the laser field and splits into three substates |α , |β , and |γ with energy V 2 + hR/2, V 2 , and V 2 − hR/2. The wave function of state |2 , including the influence of the laser field, can be expressed by dressed states |α , |β , |γ whose energies are dressed in order, [25,29]…”