Abstract:We develop necessary and sufficient conditions for the a.s. asymptotic stability of solutions of a scalar, non-linear stochastic equation with state-independent stochastic perturbations that fade in intensity. These conditions are formulated in terms of the intensity function: roughly speaking, we show that as long as the perturbations fade quicker than some identifiable critical rate, the stability of the underlying deterministic equation is unaffected. These results improve on those of Chan and Williams; for… Show more
“…The Lipschitz continuity of f , the property (1.4), (4.5), and the fact that g is continuous on [0, ∞) and g(t) → 0 as t → ∞ means, by a result in [7], that z(t) → 0 as t → ∞. This allows us to conclude that x(t) → 0 as t → ∞, as claimed.…”
This paper develops necessary and sufficient conditions for the preservation of asymptotic convergence rates of deterministically and stochastically perturbed ordinary differential equations with regularly varying nonlinearity close to their equilibrium. Sharp conditions are also established which preserve the asymptotic behaviour of the derivative of the underlying unperturbed equation. Finally, necessary and sufficient conditions are established which enable finite difference approximations to the derivative in the stochastic equation to preserve the asymptotic behaviour of the derivative of the unperturbed equation, even though the solution of the stochastic equation is nowhere differentiable, almost surely.
“…The Lipschitz continuity of f , the property (1.4), (4.5), and the fact that g is continuous on [0, ∞) and g(t) → 0 as t → ∞ means, by a result in [7], that z(t) → 0 as t → ∞. This allows us to conclude that x(t) → 0 as t → ∞, as claimed.…”
This paper develops necessary and sufficient conditions for the preservation of asymptotic convergence rates of deterministically and stochastically perturbed ordinary differential equations with regularly varying nonlinearity close to their equilibrium. Sharp conditions are also established which preserve the asymptotic behaviour of the derivative of the underlying unperturbed equation. Finally, necessary and sufficient conditions are established which enable finite difference approximations to the derivative in the stochastic equation to preserve the asymptotic behaviour of the derivative of the unperturbed equation, even though the solution of the stochastic equation is nowhere differentiable, almost surely.
“…Suppose that f obeys (2.2), g obeys (2. 3), and that f obeys (2.22) and g and f obey (2.25). Suppose that x is the unique continuous solution of (2.1).…”
Section: Precise Statement Of Main Resultsmentioning
confidence: 99%
“…in the case when g obeys (2.8) but g ∈ L 1 (0, ∞) and when f obeys (2.2) but the restoring force f (x) as x → ∞ is so weak that lim x→∞ f (x) = 0 (2.11) are presented in Appleby, Gleeson and Rodkina [3]. However, when (2.11) is strengthened so that in addition to (2.2), f also obeys There exists φ > 0 such that φ := lim inf |x|→∞ |f (x)|, (2.12) then the condition (2.8) on g suffices to ensure that the solution x of (2.1) obeys (2.6).…”
Section: 2mentioning
confidence: 99%
“…However, when (2.11) is strengthened so that in addition to (2.2), f also obeys There exists φ > 0 such that φ := lim inf |x|→∞ |f (x)|, (2.12) then the condition (2.8) on g suffices to ensure that the solution x of (2.1) obeys (2.6). See also [3]. For this reason, we restrict our focus in this paper to the case when f obeys (2.11).…”
Section: 2mentioning
confidence: 99%
“…The motivation for this work originates from work on the asymptotic behaviour of stochastic differential equations with state independent perturbations, for which the underlying deterministic equation is globally asymptotically stable. In the case when f has relatively strong mean reversion, it is shown in [3], for a sufficiently rapidly decaying noise intensity, that solutions are still asymptotically stable, but that slower convergence leads to unbounded solutions. A complete categorisation of the asymptotic behaviour in the linear case is given in [1].…”
Section: Introduction and Connection With The Literaturementioning
In this paper we consider the global and local stability and instability of solutions of a scalar nonlinear differential equation with non-negative solutions. The differential equation is a perturbed version of a globally stable autonomous equation with unique zero equilibrium where the perturbation is additive and independent of the state. It is assumed that the restoring force is asymptotically negligible as the solution becomes large, and that the perturbation tends to zero as time becomes indefinitely large. It is shown that solutions are always locally stable, and that solutions either tend to zero or to infinity as time tends to infinity. In the case when the perturbation is integrable, the zero solution is globally asymptotically stable. If the perturbation is non-integrable, and tends to zero faster than a critical rate which depends on the strength of the restoring force, then solutions are globally stable. However, if the perturbation tends to zero more slowly than this critical rate, and the initial condition is sufficiently large, the solution tends to infinity. Moreover, for every initial condition, there exists a perturbation which tends to zero more slowly than the critical rate, for which the solution once again escapes to infinity. Some extensions to general scalar equations as well as to finitedimensional systems are also presented, as well as global convergence results using Liapunov techniques.1991 Mathematics Subject Classification. Primary: 34D05, 34D23, 34D20, 34C11.
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