“…2) are typically approximated by point sources, positioned at the locations m s of the boundary, firing at the moments t 0 , and possessing infinitely short time constants: (5) Sources q p (r s , t) inside the medium [Eq. (2)] are represented by the functions of the probe absorption coefficient μ a p (r s , λ ex ), the probe quantum yield ϕ 0 in the absence of oxygen, 37 the distribution of the excitation photon density U ex (r s , t), and the lifetime τ(r s ): (6) The absorption coefficient μ a p (r s , λ ex ) is the product of the probe concentration c(r s ) and the probe molar extinction coefficient ε(λ ex ).…”