2015
DOI: 10.1016/j.amc.2015.05.082
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Fixed points of a destabilized Kuramoto–Sivashinsky equation

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Cited by 4 publications
(8 citation statements)
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“…This evolution equation is based on the gradient in the H −1 -topology and uses homogeneous Neumann boundary conditions for both u and ∆u. The diblock copolymer model (2) is an extension of the celebrated Cahn-Hilliard equation [6], which corresponds to the special case σ = 0 and serves as a fundamental model for the phase separation phenomena spinodal decomposition [31,32,44,45,52] and nucleation [3,4,18]. The quantity µ average of the solution over the domain is conserved in time.…”
Section: The Diblock Copolymer Model Description and The Main Resultsmentioning
confidence: 99%
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“…This evolution equation is based on the gradient in the H −1 -topology and uses homogeneous Neumann boundary conditions for both u and ∆u. The diblock copolymer model (2) is an extension of the celebrated Cahn-Hilliard equation [6], which corresponds to the special case σ = 0 and serves as a fundamental model for the phase separation phenomena spinodal decomposition [31,32,44,45,52] and nucleation [3,4,18]. The quantity µ average of the solution over the domain is conserved in time.…”
Section: The Diblock Copolymer Model Description and The Main Resultsmentioning
confidence: 99%
“…But how does this multistability manifest itself in the evolution equation (2)? Based on the underlying physical situation, one is usually interested in studying the long-term behavior of solutions of the diblock copolymer model which originate close to the (unstable) homogeneous equilibrium state u ≡ µ.…”
Section: The Diblock Copolymer Model Description and The Main Resultsmentioning
confidence: 99%
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