“…The same analyses we have done in this work can be easily generalized and incorporated into those alternative ET rate theories to describe PMET processes. Here, we only briefly mention some of these theories: (i) to incorporate nuclear quantum effects from high-frequency vibrational modes, one can explicitly include the quantized vibrational states by using the Jortner theory, [125][126][127] or using the linearized path-integral Fermi's golden rule (FGR) rate expressions, [128][129][130] the state-dependent imaginary-time path integral approaches, [131][132][133][134][135] or the state-dependent Instanton theory, [136][137][138] (ii) to obtain accurate rate from the weak to strong electronic coupling regimes, one can use the state-dependent Instanton theory, 136,138,139 or compute rate through the fluxside correlation function 140 using linearized pathintegral approach, 141,142 state-dependent ringpolymer rate approaches, 133,134 or mixed quantumclassical approaches, [143][144][145][146][147][148][149][150] (iii) to incorporate memory effects of the bath, one can use the Zusman theory 151 that provides accurate non-markovian and non-adiabatic ET rate, [151][152][153][154] or use the linearized path-integral FGR rate expressions, [128][129][130] (iv) to treat non-equilibrium initial condition, one can employ the recently developed non-equilibrium FGR rate theory…”