Abstract
The global existence and stability of the solution to the delay differential equation (*)$\dot{u} = A(t)u + G(t,u(t-\tau)) + f(t)$, $t\ge 0$, $u(t) = v(t)$, $-\tau \le t\le 0$, are studied. Here $A(t):\mathcal{H}\to \mathcal{H}$ is a closed, densely defined, linear operator in a Hilbert space $\mathcal{H}$ and $G(t,u)$ is a nonlinear operator in $\mathcal{H}$ continuous with respect to $u$ and $t$. We assume that the spectrum of $A(t)$ lies in the half-plane $\Re \lambda \le \gamma(t)$, where $\gamma(t)$ is not necessarily negative and $\|G(t,u)\| \le \alpha(t)\|u\|^p$, $p>1$, $t\ge 0$. Sufficient conditions for the solution to the equation to exist globally, to be bounded and to converge to zero as $t$ tends to $\infty$, under the non-classical assumption that $\gamma(t)$ can take positive values, are proposed and justified.
Highlights
Consider the following delay differential equation u = A(t)u + G(t, u(t − τ )) + f (t), t ≥ 0, u :=du dt (1a) u(t) = v(t), −τ ≤ t ≤ 0, τ = const > 0, v(t) ∈ C([−τ, 0]; H). (1b)Reference to equation (1) means reference to both equations (1a) and (1b)
If A(t) is a square matrix, the condition γ(t) ≤ γ0 < 0 implies that all the eigenvalues of A(t) lie in the half-plane Re λ ≤ γ0 < 0
The main tool for the study of the stability in [6], [7], and [9] under these non-classical assumptions is some nonlinear inequalities. These inequalities were used in the study of the Dynamical Systems Method (DSM) for solving operator equations in
Summary
The global existence and stability of the solution to the delay differential equation (*)u = A(t)u + G(t, u(t − τ )) + f (t), t ≥ 0, u(t) = v(t), −τ ≤ t ≤ 0, are studied. Using a nonlinear inequality with delay, the global existence and stability of equation (1) were studied in [10] for the case when f (t) = 0 and G(t, u) is of the form B(t)F (t, u) under the non-classical assumption that (2) holds but the inequality γ(t) ≤ γ0 < 0 does not hold for any γ0 < 0. In [10] the stability of the solution to the following differential equation with delay was studied: u = A(t)u + B(t)F (t, u(t − τ )), t ≥ 0, u u(t) = v(t), −τ ≤ t ≤ 0, τ = const > 0.
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