Interestingly, a comparison of the trap-state feature signal at 1.7 ns reveals a relatively minor dependence on intensity. In Fig. , we compare the signal between low (50W) and high (360W) excitation. Despite a more than seven-fold increase in excitation intensity, the initial GSB increases proportionally, while the trap-state signal only doubles. This suggests a limited number of traps that can be populated from the initial excited state. A similar observation is made when the excitation is changed from 610 nm to 510 nm, where the sample's higher absorption leads to a greater initial excited state population and GSB signal. However, the trapstate signal remains consistent with that observed with 610 nm excitation. Following the SSCP protocol, the initial GSB signal experiences a slight blueshift to 614 nm, with only one spectral component observed (refer to Fig. and). Simultaneously, the GSB signal decays with an average lifetime of 31 ps, an order of magnitude slower compared to the untreated samples.