2010
DOI: 10.1051/cocv/2010024
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Asymptotic behavior of second-order dissipative evolution equations combining potential with non-potential effects

Abstract: Abstract.In the setting of a real Hilbert space H, we investigate the asymptotic behavior, as time t goes to infinity, of trajectories of second-order evolution equationswhere ∇φ is the gradient operator of a convex differentiable potential function φ : H → R, A : H → H is a maximal monotone operator which is assumed to be λ-cocoercive, and γ > 0 is a damping parameter. Potential and non-potential effects are associated respectively to ∇φ and A. Under condition λγ 2 > 1, it is proved that each trajectory asymp… Show more

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Cited by 39 publications
(43 citation statements)
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“…Inertial dynamics and cocoercive operators. In analogy with (3),Álvarez-Attouch [2] and Attouch-Maingé [7] studied the equation (7)ẍ(t) + γẋ(t) + A(x(t)) = 0, where A is a cocoercive operator. Cocoercivity plays an important role, not only to ensure the existence of solutions, but also in analyzing their long-term behavior.…”
Section: Introductionmentioning
confidence: 99%
“…Inertial dynamics and cocoercive operators. In analogy with (3),Álvarez-Attouch [2] and Attouch-Maingé [7] studied the equation (7)ẍ(t) + γẋ(t) + A(x(t)) = 0, where A is a cocoercive operator. Cocoercivity plays an important role, not only to ensure the existence of solutions, but also in analyzing their long-term behavior.…”
Section: Introductionmentioning
confidence: 99%
“…In view of the Lipschitz continuity of ∇Ψ, ∇ 2 Ψ and ∇Φ, ∇ 2 Φ, assumed in (H Ψ ) and (H Φ ), respectively, the existence and uniqueness of strong global solutions of (11) is a consequence of the Cauchy-Lipschitz-Picard Theorem (see for example [5,17,25,31]).…”
Section: Preliminariesmentioning
confidence: 99%
“…The similarity between second-order Hamiltonian systems and the corresponding first-order gradient flows is wellknown in mechanical control systems [19], in dynamic optimization [20], [21], [22], and also in transient stability studies [23], [24], [25], but we are not aware of any result as general as Theorem III.1. In [23], [24], [25], statements 1) and 2) are proved under the more stringent assumptions that H λ has a finite number of isolated and hyperbolic equilibria.…”
Section: Parameterized Hamiltonian and Gradient-like Dynamics Anmentioning
confidence: 99%
“…Additionally, if H(x) constitutes an energy function and if a one-parameter transversality condition is satisfied, then the separatrices of system (6) can also be characterized accurately [23], [24], [26]. Also statement 3) can be refined under further structural assumptions on the potential function H(x), and various other minimizing properties can be deduced from the dynamics (6), see [19], [20], [21], [22].…”
Section: Parameterized Hamiltonian and Gradient-like Dynamics Anmentioning
confidence: 99%