FCS analysis of QDs is fundamentally different from that of organic dye molecules. The blinking of a dye molecule is caused by the participation of triplet states, where the timescale of blinking is precisely described by a single time constant without the need for a distribution parameter. Conversely, QD blinking does not adhere to a specific time constant; instead, it is distributed across all timescales. This prompted us to use a distribution parameter β in the fitting equation of the FCS curves of our d-PNCs. Even the fitting with our modified fitting equation cannot provide an accurate blinking timescale of d-PNCs due to its non-convergent nature. In fact, it was observed that a significantly extended observation window (~≤440 ms) was found insufficient to achieve convergence of τR. This suggests that the carrier dynamics in d-PNCs proceed on timescales that could potentially extend to seconds or even longer durations.