“…The more recent dynamic versions of the classical POT model found in several studies (i.e., [ 4 , 5 , 6 , 7 , 8 , 9 , 10 , 11 , 12 , 13 , 14 ]), are directly motivated by the behavior of the non-homogeneous Poisson point process, where the intensity rate of threshold exceedances, , can vary over time due to the temporal bursts in volatility. According to such a point process approach to POT models, the first factor on the left-hand side of Equation ( 3 ) (i.e., the conditional probability of a threshold exceedance over day ) can be derived based on the (time varying) conditional intensity function as follows: because the probability of no events in (i.e., ) can be given as [ 21 ].…”