2011
DOI: 10.4171/ifb/260
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A semidiscrete scheme for a one-dimensional Cahn–Hilliard equation

Abstract: We analyze a semidiscrete scheme for the Cahn-Hilliard equation in one space dimension, when the interface length parameter is equal to zero. We prove convergence of the scheme for a suitable class of initial data, and we identify the limit equation. We also characterize the long-time behavior of the limit solutions.

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Cited by 7 publications
(6 citation statements)
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“…In the case of hysteretic interface motion, there seems to be no rigorous result -neither for the lattice nor the viscous approximation -that derives (1.9) and (1.10) rigorously from the dynamics for ε > 0. Previous results for the lattices (1.1) or (1.2) are either restricted to standing interfaces, see [GN11] and [BGN13] for type-I and type-II interfaces, respectively, or do not capture the dynamics of moving interfaces completely, e. g. [BNP06].…”
Section: A the Discrete Heat Kernel 1 Introductionmentioning
confidence: 99%
“…In the case of hysteretic interface motion, there seems to be no rigorous result -neither for the lattice nor the viscous approximation -that derives (1.9) and (1.10) rigorously from the dynamics for ε > 0. Previous results for the lattices (1.1) or (1.2) are either restricted to standing interfaces, see [GN11] and [BGN13] for type-I and type-II interfaces, respectively, or do not capture the dynamics of moving interfaces completely, e. g. [BNP06].…”
Section: A the Discrete Heat Kernel 1 Introductionmentioning
confidence: 99%
“…We observe that equation (1.1) is not the only way to regularize the ill-posed gradient flow equation of the functional (1.4): other regularizations have been considered in the literature, see for instance [15,7,10,9,19]. In particular, in [7] it is proposed an implicit variational scheme for the functional (1.4) which converges to (1.6) as the discretization parameter tends to zero.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, for initial data with p j (0) < p * for all j ∈ Z no u j can reach the spinodal region from below, and if p j (0) ∈ [p * , p * ] then no interface moves at all. See Geldhauser and Novaga (2011) or Helmers and Herrmann (2013) for more details.…”
Section: Microscopic Interface Dynamicsmentioning
confidence: 99%
“…The case of standing interfaces is much simpler and has been settled in Geldhauser and Novaga (2011) by localizing standard methods for parabolic PDEs.…”
Section: Rigorous Justification Of the Limitmentioning
confidence: 99%