TY - JOUR
T1 - Predicting the last zero before an exponential time of a spectrally negative Lévy process
AU - Pedraza Ramirez, Jose M.
AU - Baurdoux, Erik
PY - 2023/6/1
Y1 - 2023/6/1
N2 - Given a spectrally negative Lévy process, we predict, in an $L_p$sense, the last passage time of the process below zero before an independent exponential time. This optimal prediction problem generalises [2], where the infinite-horizon problem is solved. Using a similar argument as that in [24], we show that this optimal prediction problem is equivalent to solving an optimal prediction problem in a finite-horizon setting. Surprisingly (unlike the infinite-horizon problem), an optimal stopping time is based on a curve that is killed at the moment the mean of the exponential time is reached. That is, an optimal stopping time is the first time the process crosses above a non-negative, continuous, and non-increasing curve depending on time. This curve and the value function are characterised as a solution of a system of nonlinear integral equations which can be understood as a generalisation of the free boundary equations (see e.g. [21, Chapter IV.14.1]) in the presence of jumps. As an example, we numerically calculate this curve in the Brownian motion case and for a compound Poisson process with exponential-sized jumps perturbed by a Brownian motion.
AB - Given a spectrally negative Lévy process, we predict, in an $L_p$sense, the last passage time of the process below zero before an independent exponential time. This optimal prediction problem generalises [2], where the infinite-horizon problem is solved. Using a similar argument as that in [24], we show that this optimal prediction problem is equivalent to solving an optimal prediction problem in a finite-horizon setting. Surprisingly (unlike the infinite-horizon problem), an optimal stopping time is based on a curve that is killed at the moment the mean of the exponential time is reached. That is, an optimal stopping time is the first time the process crosses above a non-negative, continuous, and non-increasing curve depending on time. This curve and the value function are characterised as a solution of a system of nonlinear integral equations which can be understood as a generalisation of the free boundary equations (see e.g. [21, Chapter IV.14.1]) in the presence of jumps. As an example, we numerically calculate this curve in the Brownian motion case and for a compound Poisson process with exponential-sized jumps perturbed by a Brownian motion.
KW - Lévy processes
KW - optimal prediction
KW - optimal stopping
UR - http://www.scopus.com/inward/record.url?scp=85159298176&partnerID=8YFLogxK
UR - https://www.mendeley.com/catalogue/d53dcf43-6401-305b-b22b-f835b729cd0f/
U2 - 10.1017/apr.2022.47
DO - 10.1017/apr.2022.47
M3 - Article
SN - 0001-8678
VL - 55
SP - 611
EP - 642
JO - Advances in Applied Probability
JF - Advances in Applied Probability
IS - 2
ER -