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

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Summary

Introduction

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.

Results
Conclusion

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