For processes $X(t),t>0$ governed by signed measures whose density is the fundamental solution of third and fourth-order heat-type equations (higher-order diffusions) the explicit form of the joint distribution of $(\max_{0\leqs\leqt}X(s),X(t))$ is derived. The expressions presented include all results obtained so far and, for the third-order case, prove to be genuine probability distributions. The case of more general fourth-order equations is also investigated and the distribution of the maximum is derived
We give a direct derivation of the distribution of the maximum and the location of the maximum of on...
Let T be the first time a stochastic process {X(t)} drops a units below its maximum to date. We dete...
Consider a one dimensional diffusion process on the diffusion interval I originated in x0 ∈ I. Let a...
AbstractThe conditional Feynman–Kac functional is used to derive the Laplace transforms of condition...
The conditional Feynman-Kac functional is used to derive the Laplace transforms of conditional maxim...
Consider the Slepian process S defined by S(t) = B(t + 1) − B(t),t ∈ [0, 1] with B(t), t ∈ ℝ a stand...
Abstract. In this paper we introduce new distributions which are solutions of higher-order Laplace e...
25 pagesInternational audienceLet $(X(t))_{t \ge 0}$ be the pseudo-process driven by the high-order ...
Let X be a d-dimensional diffusion process and M the running supremum of the first component. In thi...
In contrast to the classical theory of partial sums of independent and identically distributed rando...
In this paper we are interested in the distribution of the maximum, or the maximum of the absolute v...
For the fundamental solutions of heat-type equations of order n we give a general stochastic represe...
Abstract. For the fundamental solutions of heat-type equations of order n we give a general stochast...
AbstractWe derive estimates of solutions of the semilinear 2mth-order parabolic equation of diffusio...
Consider a Lévy process with finite intensity positive jumps of the phase-type and arbitrary negati...
We give a direct derivation of the distribution of the maximum and the location of the maximum of on...
Let T be the first time a stochastic process {X(t)} drops a units below its maximum to date. We dete...
Consider a one dimensional diffusion process on the diffusion interval I originated in x0 ∈ I. Let a...
AbstractThe conditional Feynman–Kac functional is used to derive the Laplace transforms of condition...
The conditional Feynman-Kac functional is used to derive the Laplace transforms of conditional maxim...
Consider the Slepian process S defined by S(t) = B(t + 1) − B(t),t ∈ [0, 1] with B(t), t ∈ ℝ a stand...
Abstract. In this paper we introduce new distributions which are solutions of higher-order Laplace e...
25 pagesInternational audienceLet $(X(t))_{t \ge 0}$ be the pseudo-process driven by the high-order ...
Let X be a d-dimensional diffusion process and M the running supremum of the first component. In thi...
In contrast to the classical theory of partial sums of independent and identically distributed rando...
In this paper we are interested in the distribution of the maximum, or the maximum of the absolute v...
For the fundamental solutions of heat-type equations of order n we give a general stochastic represe...
Abstract. For the fundamental solutions of heat-type equations of order n we give a general stochast...
AbstractWe derive estimates of solutions of the semilinear 2mth-order parabolic equation of diffusio...
Consider a Lévy process with finite intensity positive jumps of the phase-type and arbitrary negati...
We give a direct derivation of the distribution of the maximum and the location of the maximum of on...
Let T be the first time a stochastic process {X(t)} drops a units below its maximum to date. We dete...
Consider a one dimensional diffusion process on the diffusion interval I originated in x0 ∈ I. Let a...