The spectrum taken after the 2% pulse had substantially higher intensity, and fitting gave TNP (averaged over the 2 NPs) of 1287 K, i.e., the same 532 nm heating power gave higher TNP despite the fact that the emission intensity, hence the radiative cooling, roughly doubled. This implies that the absorptivity at 532 nm had increased more than enough to compensate for the greater radiative cooling. The trap contents were then briefly heated two more times at 3% and 4% duty factor, respectively, and even though one NP appears to have been lost (or shifted out of the Fz scan range) during the 3% flash, the emission intensity and extracted TNP values continued to increase. From the size of the Fz steps, we roughly estimate that the mass of the surviving NP was ~138 MDa, compared to the ~5.5 MDa mass expected for individual particles of the nominally ~20 nm diameter feedstock, i.e., this NP was certainly an aggregate particle, and therefore fission may well have occurred.