“…Similarly, the conversion could also be achieved by applying optical pulses with different frequencies and numbers (Figure 2h,i). To further evaluate the conversion process from STM to LTM, a typical stretched exponential function was introduced to fit the decay curves: [
54,55 ]
where I 0 , t 0 , τ , β , and I ∞ denoted the maximum photocurrent, the ending time of the optical pulse, the decay time, the stretch index between 0 and 1, and the background current, respectively. Figure S6 (Supporting Information) displays the gradual increase of τ with the increase of width, frequency, and number of the optical pulses, further demonstrating the conversion process from STM to LTM.…”