“…For example, there are several papers (see e.g. [26,47,[71][72][73][74][75]) dedicated to analyzing the optical behavior of quantum dots by calculating the absorption coefficient, 𝜁, and the relative changes at the same order of the refractive index, ∆𝑛∕𝑛, for an incident linearly polarized light beam. For a transition (𝓀 𝑖 , 𝓁 𝑖 , 𝓃 𝑖 ) → (𝓀 𝑗 , 𝓁 𝑗 , 𝓃 𝑗 ), we can compute such quantities (at first order for simplicity) as functions of the energy 𝐸 𝛾 of the incident photon [26] by using a density matrix approach and a perturbation expansion method [76] Here, 𝜇 0 is the permeability of the vacuum, 𝜀 = 𝜀 0 𝑛 2 𝑟 = 𝜀 0 𝜀 𝑟 is the real part of the permittivity of the material (𝜀 0 is the permittivity of the vacuum, 𝜀 𝑟 is the static dielectric constant of the material and 𝑛 𝑟 = √ 𝜀 𝑟 is the refractive index of the medium), 𝜎 𝑣 is the carrier density, Γ 𝑖𝑗 = ℏ∕𝑇 𝑖𝑗 is the relaxation rate-is a damping-related Lorentzian term associated with exciton scattering losses in the system [73]-(𝑇 𝑖𝑗 is the time relaxation), ℳ 𝑎;𝑖𝑗 ≡ ⟨Ψ 𝑎;𝓀 𝑗 ,𝓁 𝑗 ,𝓃 𝑗 |𝑒𝑥| Ψ 𝑎;𝓀 𝑖 ,𝓁 𝑖 ,𝓃 𝑖 ⟩ is the dipole matrix element for 𝑥-polarized incident radiation (𝑒 is the elementary charge) and ∆𝐸 𝑎;𝑖𝑗 ≡ 𝐸 𝑎;𝓀 𝑗 ,𝓁 𝑗 ,𝓃 𝑗 − 𝐸 𝑎;𝓀 𝑖 ,𝓁 𝑖 ,𝓃 𝑖 is the energy gap between the levels.…”