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1.
We wish to characterize when a Lévy process X t crosses boundaries b(t), in a two-sided sense, for small times t, where b(t) satisfies very mild conditions. An integral test is furnished for computing the value of sup t→0|X t |/b(t) = c. In some cases, we also specify a function b(t) in terms of the Lévy triplet, such that sup t→0 |X t |/b(t) = 1.  相似文献   

2.
In this article, the inverse problem of the differential inclusion theory is studied. For a given ε>0 and a continuous set valued map tW(t), t∈[t0,θ], where W(t)⊂Rn is compact and convex for every t∈[t0,θ], it is required to define differential inclusion so that the Hausdorff distance between the attainable set of the differential inclusion at the time moment t with initial set (t0,W(t0)) and W(t) would be less than ε for every t∈[t0,θ].  相似文献   

3.
Let Xt be n-dimensional diffusion process and St be a smooth set-valued function. Suppose Xt is invisible when XtSt, but we can see the process exactly otherwise. Let Xt0St0 and we observe the process from the beginning till the signal reappears out of the obstacle after t0. With this information, we evaluate the estimators for the functionals of Xt on a time interval containing t0 where the signal is hidden. We solve related 3 PDEs in general cases. We give a generalized last exit decomposition for n-dimensional Brownian motion to evaluate its estimators. An alternative Monte Carlo method is also proposed for Brownian motion. We illustrate several examples and compare the solutions between those by the closed form result, finite difference method, and Monte Carlo simulations.  相似文献   

4.
It is shown that the trivariate stochastic processes {(MtWt, Mt, Θt), t ≥ 0} and {(|Wt|, Lt, Tt), t ≥ 0} have the same distributions when: W = {Wt, t ≥ 0} is a Wiener process, Mt is the maximum value attained by W over the time interval [0, t], Θt is the time the maximum value is attained, Lt is the local time of W at level zero and time t, and Tt is the last time W is zero in the time interval [0, t]. A straightforward proof, based on ‘Tanaka's formula, establishes this result by deriving an almost sure version of the equivalence.  相似文献   

5.
The following first order nonlinear differential equation with a deviating argument $ x'(t) + p(t)[x(\tau (t))]^\alpha = 0 $ is considered, where α > 0, α ≠ 1, pC[t 0; ∞), p(t) > 0 for tt 0, τC[t 0; ∞), lim t→∞ τ(t) = ∞, τ(t) < t for tt 0. Every eventually positive solution x(t) satisfying lim t→∞ x(t) ≧ 0. The structure of solutions x(t) satisfying lim t→∞ x(t) > 0 is well known. In this paper we study the existence, nonexistence and asymptotic behavior of eventually positive solutions x(t) satisfying lim t→∞ x(t) = 0.  相似文献   

6.
The asymptotic distribution of the maximum Mn=max1?t?nξt in a stationary normal sequence ξ1,ξ,… depends on the correlation rt between ξ0 and ξt. It is well known that if rt log t → 0 as t → ∞ or if Σr2t<∞, then the limiting distribution is the same as for a sequence of independent normal variables. Here it is shown that this also follows from a weaker condition, which only puts a restriction on the number of t-values for which rt log t islarge. The condition gives some insight into what is essential for this asymptotic behaviour of maxima. Similar results are obtained for a stationary normal process in continuous time.  相似文献   

7.
Let {Xt} be a continuous square integrable martingale. Denote its increasing (natural) process by {At}. Let St, Tt be the left and right inverses of At, respectively. Then for any square integrable martingale {Yt} defined on {Xt}, Yt = ∝0tψsdXs, R0 < t < S where S = limt→∞St, R0 = inf {t: Xt ≠ 0} provided that Y(T(t)) is σ(X(T(s)): s ? t)-measurable. All martingales are assumed to be zero at t = 0. Brownian motion and Poisson processes are considered also.  相似文献   

8.
A necessary and sufficient condition is given for the convergence in probability of a stochastic process {Xt}. Moreover, as a byproduct, an almost sure convergent stochastic process {Yt} with the same limit as {Xt} is identified. In a number of cases {Yt} reduces to {Xt} thereby proving a.s. convergence. In other cases it leads to a different sequence but, under further assumptions, it may be shown that {Xt} and {Yt} are a.s. equivalent, implying that {Xt} is a.s. convergent. The method applies to a number of old and new cases of branching processes providing an unified approach. New results are derived for supercritical branching random walks and multitype branching processes in varying environment.  相似文献   

9.
The oscillatory nature of two equations (r(t) y′(t))′ + p1(t)y(t) = f(t), (r(t) y′(t))′ + p2(t) y(t ? τ(t))= 0, is compared when positive functions p1 and p2 are not “too close” or “too far apart.” Then the main theorem states that if h(t) is eventually negative and a twice continuously differentiable function which satisfies (r(t) h′(t))′ + p1(t) h(t) ? 0, then this inequality is necessary and sufficient for every bounded solution of (r(t) y′(t))′ + p2(t) y(t ? τ(t)) = 0 to be nonoscillatory.  相似文献   

10.
11.
A deterministic version of the Itô calculus is presented. We consider a modelY t=H(N t ,t) with a deterministic Brownian N t and an unknown functionH. We predictY c from the observation {Y t;t ∈ [a, b]}, wherea. We prove that there exists an estimatorY t based on the observation such thatE[(? t?Y c)2]=O((c?b)2) ascb.  相似文献   

12.
Let A(t) be a complex Wishart process defined in terms of the M×N complex Gaussian matrix X(t) by A(t)=X(t)X(t)H. The covariance matrix of the columns of X(t) is Σ. If X(t), the underlying Gaussian process, is a correlated process over time, then we have dependence between samples of the Wishart process. In this paper, we study the joint statistics of the Wishart process at two points in time, t1, t2, where t1<t2. In particular, we derive the following results: the joint density of the elements of A(t1), A(t2), the joint density of the eigenvalues of Σ-1A(t1),Σ-1A(t2), the characteristic function of the elements of A(t1), A(t2), the characteristic function of the eigenvalues of Σ-1A(t1),Σ-1A(t2). In addition, we give the characteristic functions of the eigenvalues of a central and non-central complex Wishart, and some applications of the results in statistics, engineering and information theory are outlined.  相似文献   

13.
Let X(t) and Y(t) be two stochastically continuous processes with independent increments over [0, T] and Lévy spectral measures Mt and Nt, respectively, and let the “time-jump” measures M and N be defined over [0, T] × R?{0} by M((t1, t2] × A) = Mt2(A) ? Mt1(A) and N((T1, t2] × A) = Nt2(A) ? Nt1(A). Under the assumption that M is equivalent to N, it is shown that the measures induced on function space by X(t) and Y(t) are either equivalent or orthogonal, and necessary and sufficient conditions for equivalence are given. As a corollary a complete characterization of the set of admissible translates of such processes is obtained: a function f is an admissible translate for X(t) if and only if it is an admissible translate for the Gaussian component of X(t). In particular, if X(t) has no Gaussian component, then every nontrivial translate of X(t) is orthogonal to it.  相似文献   

14.
The unstable properties of the null solution of the nonautonomous delay system x′(t)=A(t)x(t)+B(t)x(tr1(t))+f(t,x(t),x(tr2(t))) are examined; the nonconstant delays r1, r2 are assumed to be continuous bounded functions. The case A=constant is reviewed, where a theorem, recalling the Perron instability theorem for ordinary differential equations, is obtained.  相似文献   

15.
Fix p?>?1, not necessarily integer, with p(d ? 2)?< d. We study the p-fold self-intersection local time of a simple random walk on the lattice ${\mathbb Z^d}$ up to time t. This is the p-norm of the vector of the walker??s local times, ? t . We derive precise logarithmic asymptotics of the expectation of exp{?? t ||? t || p } for scales ?? t >?0 that are bounded from above, possibly tending to zero. The speed is identified in terms of mixed powers of t and ?? t , and the precise rate is characterized in terms of a variational formula, which is in close connection to the Gagliardo?CNirenberg inequality. As a corollary, we obtain a large-deviation principle for ||? t || p /(tr t ) for deviation functions r t satisfying ${t r_t\gg \mathbb E[||\ell_t||_p]}$ . Informally, it turns out that the random walk homogeneously squeezes in a t-dependent box with diameter of order ? t 1/d to produce the required amount of self-intersections. Our main tool is an upper bound for the joint density of the local times of the walk.  相似文献   

16.
Oscillation criteria for the class of forced functional differential inequalities x(t){Lnx(t) + f(t, x(t), x[g1(t)],…, x[gm(t)]) ? h(t)} ? 0, for n even, and x(t){Lnx(t) ? f(t, x(t), x[g1(t)],…, x[gm(t)]) ? h(t)} ? 0, for n odd, are established.  相似文献   

17.
Differential equations ·x(t) = f(x(t), t) are exhibited in a general infinite-dimensional Banach space, failing each of the following in turn. (i) The set St of solution values x(t) from a given point x(0) is compact. (ii) St is connected. (iii) Any point on the boundary ?St of St can be reached by a solution x with x(s) ??Ss, 0 ? s ? t.  相似文献   

18.
For the Cauchy problem, ut = uxx, 0 < x < 1, 0 < t ? T, u(0, t) = f(t), 0 < t ? T, ux(0, t) = g(t), 0 < t ? T, a direct numerical procedure involving the elementary solution of υt = υxx, 0 < x, 0 < t ? T, υx(0, t) = g(t), 0 < t ? T, υ(x, 0) = 0, 0 < x and a Taylor's series computed from f(t) ? υ(0, t) is studied. Continuous dependence better than any power of logarithmic is obtained. Some numerical results are presented.  相似文献   

19.
This Note presents a construction of a solution for the nonlinear stochastic differential equation Xt = X0 + ∫0t E[u0(X0)|Xs]ds, t ≥ 0. The random variable X0 with values in R and the function u0 are given. We denote by Pt the probability distribution of Xt and u(x, t) = E[u0(X0)|Xt = x]. We prove that (Pt, u(·, t), t ≥ 0) is a weak solution for system of conservation law arising in adhesion particle dynamics.  相似文献   

20.
In this paper, we consider the Hele-Shaw problem in a 2-dimensional fluid domain Ω(t) which is constrained to a half-plane. The boundary of Ω(t) consist of two components: Γ0(t) which lies on the boundary of the half-plane, and Γ(t) which lies inside the half-plane. On Γ(t) we impose the classical boundary conditions with surface tension, and on Γ0(t) we prescribe the normal derivative of the fluid pressure. At the point where Γ0(t) and Γ(t) meet, there is an abrupt change in the boundary condition giving rise to a singularity in the fluid pressure. We prove that the problem has a unique solution with smooth free boundary Γ(t) for some small time interval.  相似文献   

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