“…This behavior can be explained by nuclear spin statistics: symmetric tops with three equivalent hydrogens, such as CH 3 CCH, have two different spin symmetriesnamely, A and E. The A states correlate with the transitions with K=0, 3, 6, 9, ..., whereas the E states correspond to the remaining transitions, such as K=1, 2, 4, 5, ... (e.g. Strom et al 2020). Those states have relative statistical weights of A:E = 2:1 (Herzberg 1945), and therefore the population distribution of the transitions at higher temperatures will favor the K=3 states.…”