“…A large deviation theory beyond Poissonian resetting allows to appreciate the emergence of singularities in the graph of their rate functions, which are interpreted as dynamical phase transitions. Dynamical phase transitions have been already documented for time-averaged quantities such as the heat exchanged after a quench [27,28], the heat exchanged between two thermal walls [29,30], the active work in active matter [31], the total displacement of random walks [32][33][34][35], occupation times of a Brownian particle [36,37], and the entropy production [38][39][40][41][42]. Physicists often invoke the Gärtner-Ellis theorem to justify their calculations that lead to dynamical phase transitions, although it is necessary for a dynamical phase transition to occur that the hypotheses of that theorem are violated.…”