1,721,040 research outputs found

    Inverse First-Passage Problems of a Diffusion with Resetting

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    We address some inverse problems for the first-passage place and the first-passage time of a one-dimensional diffusion process with stochastic resetting. This type of diffusion is characterized by the fact that a reset to the position xR can occur according to a homogeneous Poisson process with rate r > 0. As regards the inverse first-passage place problem, for random initial position belonging to an interval (0, b) with finite b > 0 (and fixed r and xR belonging to (0, b)), let τ be the first time at which the process exits the interval (0, b), and π0 be the probability of exit from the left end of (0, b). Given a probability q, the inverse first-passage place problem consists in finding the density g of the initial position, if it exists, such that π0 = q. Concerning the inverse first-passage time problem, for random positive starting point (and fixed r and xR > 0), let again τ be the first-passage time of the process through zero. For a given distribution function F(t) on the positive real axis, the inverse first-passage time problem consists in finding the density g of the starting point, if it exists, such that P(τ ≤ t) = F(t), t > 0. In addition to the case of random initial position, we also study the case when the initial position and the resetting rate r are fixed, whereas the reset position xR is random. For all types of inverse problems considered, several explicit examples of solutions are reported

    The first-passage area of a Wiener process with stochastic resetting

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    Some Remarks on the Mean of the Running maximum of Integrated Gauss-Markov Processes and Their First-Passage Times.

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    Explicit formulae for the mean of the running maximum of conditional and unconditional Brownian motion are found; these formulae are used to obtain the mean, a(t), of the running maximum of an integrated Gauss-Markov process X(t). Moreover, the connection between the moments of the first-passage-time of X(t) and a(t) is investigated. Some explicit examples are reported

    Stochastic Modeling in Biological System

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    On the joint distribution of first-passage time and first-passage area of drifted Brownian motion

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    For drifted Brownian motion X(t) = x − μt + Bt (μ > 0) starting from x > 0, we study the joint distribution of the first-passage time below zero, τ (x), and the firstpassage area, A(x), swept out by X till the time τ (x). In particular, we establish differential equations with boundary conditions for the joint moments E[τ (x)mA(x)n], and we present an algorithm to find recursively them, for any m and n. Finally, the expected value of the time average of X till the time τ (x) is obtaine

    On the entropy of fractionally integrated gauss–markov processes

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    This paper is devoted to the estimation of the entropy of the dynamical system {Xα (t), t ≥ 0}, where the stochastic process Xα (t) consists of the fractional Riemann–Liouville integral of order α ∈ (0, 1) of a Gauss–Markov process. The study is based on a specific algorithm suitably devised in order to perform the simulation of sample paths of such processes and to evaluate the numerical approximation of the entropy. We focus on fractionally integrated Brownian motion and Ornstein–Uhlenbeck process due their main rule in the theory and application fields. Their entropy is specifically estimated by computing its approximation (ApEn). We investigate the relation between the value of α and the complexity degree; we show that the entropy of Xα (t) is a decreasing function of α ∈ (0, 1)

    The mean of the running maximum of an integrated Gauss-Markov process and the connection with its first-passage time.

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    We find explicit formulae for the mean of the running maximum of conditional and unconditional Brownian motion; they are used to obtain the mean, a(t), of the running maximum of an integrated Gauss–Markov process. Then, we deal with the connection between the moments of its first-passage-time and a(t). As explicit examples, we consider integrated Brownian motion and integrated Ornstein–Uhlenbeck process

    An inverse first-passage problem revisited: the case of fractional Brownian motion, and time-changed Brownian motion

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    We revisit an inverse first-passage time (IFPT) problem, in the cases of fractional Brownian motion, and time-changed Brownian motion. Let X(t)X(t) be a one dimensional continuous stochastic process starting from a random position etaeta , let S(t)S(t) be an assigned continuous boundary, such that etageS(0) eta ge S(0) with probability one, and F an assigned distribution function. The IFPT problem here considered consists in finding the distribution of etaeta such that the first-passage time of X(t) below S(t) has distribution F. We study this IFPT problem for fractional Brownian motion and a constant boundary S(t)=SS(t)=S; we also obtain some extension to other Gaussian processes, for one, or two, time dependent boundaries

    On the Estimation of the Persistence Exponent for a Fractionally Integrated Brownian Motion by Numerical Simulations

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    For a fractionally integrated Brownian motion (FIBM) of order (Formula presented.) (Formula presented.) we investigate the decaying rate of (Formula presented.) as (Formula presented.) where (Formula presented.) is the first-passage time (FPT) of (Formula presented.) through the barrier (Formula presented.) Precisely, we study the so-called persistent exponent (Formula presented.) of the FPT tail, such that (Formula presented.) as (Formula presented.) and by means of numerical simulation of long enough trajectories of the process (Formula presented.) we are able to estimate (Formula presented.) and to show that it is a non-increasing function of (Formula presented.) with (Formula presented.) In particular, we are able to validate numerically a new conjecture about the analytical expression of the function (Formula presented.) for (Formula presented.) Such a numerical validation is carried out in two ways: in the first one, we estimate (Formula presented.) by using the simulated FPT density, obtained for any (Formula presented.) in the second one, we estimate the persistent exponent by directly calculating (Formula presented.) Both ways confirm our conclusions within the limit of numerical approximation. Finally, we investigate the self-similarity property of (Formula presented.) and we find the upper bound of its covariance function

    Fractionally integrated Gauss-Markov processes and applications

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    We investigate the stochastic processes obtained as the fractional Riemann-Liouville inte-gral of order alpha is an element of (0 , 1) of Gauss-Markov processes. The general expressions of the mean, variance and covariance functions are given. Due to the central role, for the fractional inte-gral of standard Brownian motion and of the non-stationary/stationary Ornstein-Uhlenbeck processes, the covariance functions are carried out in closed-form. In order to clarify how the fractional order parameter alpha affects these functions, their numerical evaluations are shown and compared also with those of the corresponding processes obtained by ordi-nary Riemann integral. The results are useful for fractional neuronal models with long range memory dynamics and involving correlated input processes. The simulation of these fractionally integrated processes can be performed starting from the obtained covariance functions. A suitable neuronal model is proposed. Graphical comparisons are provided and discussed
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