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A second-order linear energy-stable scheme for slope-selection epitaxial thin-film growth

  • Published: 14 April 2026
  • MSC : 65M06, 65N06

  • The slope-selection epitaxial thin-film growth model was formulated as the $ L^2 $-gradient flow of an energy functional with a nonlinear potential of the surface slope. We developed a second-order, linear, and energy-stable scheme for this model based on a linear convex splitting in which the nonlinear potential term was treated explicitly together with an auxiliary term that ensured the convexity of the explicit part. The scheme was constructed using a second-order strong-stability-preserving implicit–explicit Runge–Kutta method. We explicitly identified the range of Runge–Kutta coefficients for which the original discrete energy decay property held, and proved that the scheme was unconditionally energy-stable with respect to the original discrete energy functional. Numerical results were presented to verify the accuracy, computational efficiency, and long-time energy stability of the scheme.

    Citation: Hyun Geun Lee. A second-order linear energy-stable scheme for slope-selection epitaxial thin-film growth[J]. AIMS Mathematics, 2026, 11(4): 9989-10003. doi: 10.3934/math.2026412

    Related Papers:

  • The slope-selection epitaxial thin-film growth model was formulated as the $ L^2 $-gradient flow of an energy functional with a nonlinear potential of the surface slope. We developed a second-order, linear, and energy-stable scheme for this model based on a linear convex splitting in which the nonlinear potential term was treated explicitly together with an auxiliary term that ensured the convexity of the explicit part. The scheme was constructed using a second-order strong-stability-preserving implicit–explicit Runge–Kutta method. We explicitly identified the range of Runge–Kutta coefficients for which the original discrete energy decay property held, and proved that the scheme was unconditionally energy-stable with respect to the original discrete energy functional. Numerical results were presented to verify the accuracy, computational efficiency, and long-time energy stability of the scheme.



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