2020
DOI: 10.1016/j.jde.2020.02.006
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Classical bounded and almost periodic solutions to quasilinear first-order hyperbolic systems in a strip

Abstract: We consider boundary value problems for quasilinear first-order one-dimensional hyperbolic systems in a strip. The boundary conditions are supposed to be of a smoothing type, in the sense that the L 2 -generalized solutions to the initial-boundary value problems become eventually C 2 -smooth for any initial L 2 -data. We investigate small global classical solutions and obtain the existence and uniqueness result under the condition that the evolution family generated by the linearized problem has exponential di… Show more

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Cited by 7 publications
(3 citation statements)
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“…Moreover, we will use the fact that, if a function w(x, t) has bounded and continuous partial derivatives up to the second order in both x ∈ [0, 1] and in t ∈ R and is Bohr almost periodic in t uniformly in x (or, simply, almost periodic), the last property is true for ∂ x w(x, t) and ∂ t w(x, t) also. Specifically, the almost periodicity of ∂ t w(x, t) follows from [6, Theorem 2.5], while the almost periodicity of ∂ x w(x, t) is shown in [20,Section 5.2]. We are, therefore, reduced to showing that the approximating sequence V k , constructed in Sect.…”
Section: B(x T) = B(x Tṽ (X T)) Fulfill the Inequalitiesmentioning
confidence: 99%
See 1 more Smart Citation
“…Moreover, we will use the fact that, if a function w(x, t) has bounded and continuous partial derivatives up to the second order in both x ∈ [0, 1] and in t ∈ R and is Bohr almost periodic in t uniformly in x (or, simply, almost periodic), the last property is true for ∂ x w(x, t) and ∂ t w(x, t) also. Specifically, the almost periodicity of ∂ t w(x, t) follows from [6, Theorem 2.5], while the almost periodicity of ∂ x w(x, t) is shown in [20,Section 5.2]. We are, therefore, reduced to showing that the approximating sequence V k , constructed in Sect.…”
Section: B(x T) = B(x Tṽ (X T)) Fulfill the Inequalitiesmentioning
confidence: 99%
“…The smoothing property allowed us in [20] to solve the problem (1.1)- (1.3) where the boundary conditions (1.2) are specified to be of the reflection type, without the requirement of the smallness of D L(BC(Π,R n )) . In [20], we used the assumption that the evolution family generated by a linearized problem has exponential dichotomy on R and proved that the dichotomy survives under small perturbations in the coefficients of the hyperbolic system. For more general boundary conditions (in particular, for (1.2)) when the operator C is not nilpotent, the issue of the robustness of exponential dichotomy for hyperbolic PDEs remains a challenging open problem.…”
Section: Nilpotency Of the Operator Cmentioning
confidence: 99%
“…The smoothing property allowed us in [17] to solve the problem (1.1)-(1.2) where the boundary conditions (1.2) are specified to be of the reflection type, without the requirement of the smallness of D L(BC(Π,R n )) . In [17] we used the assumption that the evolution family generated by a linearized problem has exponential dichotomy on R and proved that the dichotomy survives under small perturbations in the coefficients of the hyperbolic system, see also [18]. For more general boundary conditions (in particular, for (1.2)) when the operator C is not nilpotent, the issue of the robustness of exponential dichotomy for hyperbolic PDEs remains a challenging open problem.…”
Section: Weaker Assumptions On the Operator Cmentioning
confidence: 99%