“…The optical field is modeled in eq as a periodically oscillating electric field E ( t ) = E 0 ( e iωt + e – iωt ) with amplitude E 0 and frequency ω. Its interaction with the transition dipole moment d 01 of the states | 0, S 0 ⟩ and | 0, S 1 ⟩ leads to the stimulated absorption and emission processes, whose rates, k 0, S 1 ← 0, S 0 field and k 0, S 0 ← 0, S 1 field , are equal in magnitude and given by , where the energy gap is ℏω 10 = E 0, S 1 – E 0, S 0 and the broadening κ 0 S 1 ,0 S 0 is caused by the electron transfer processes between the neutral singlet states and the other charged states. , For simplicity, we denote the rate k 0, S 0 ↔0, S 1 field as k field from now on. The rate of spontaneous emission process k 0, S 0 ← 0, S 1 spon is considered in our model phenomenologically and calculated as − , where α is the fine structure constant, n is the refractive index, and c is the speed of light in vacuum.…”