[Paper Review] Stability of solutions to nonlinear diffusion equations
This paper establishes the stability of solutions to nonlinear diffusion equations—specifically the porous medium and fast diffusion equations—under perturbations in the nonlinearity exponent $ m $, using elementary estimates based on weak solutions and compactness. It proves that solutions converge in $ L^{1+m} $ norm as $ m_i \to m $, even across degenerate ($ m>1 $) and singular ($ m<1 $) regimes, without relying on regularity theory or semigroup methods.
We prove stability results for nonlinear diffusion equations of the porous medium and fast diffusion types with respect to the nonlinearity power $m$: solutions with fixed data converge in a suitable sense to the solution of the limit problem with the same data as $m$ varies. Our arguments are elementary and based on a general principle. We use neither regularity theory nor nonlinear semigroups, and our approach applies to e.g. Dirichlet problems in bounded domains and Cauchy problems on the whole space.
Motivation & Objective
- To establish the stability of solutions to nonlinear diffusion equations with respect to variations in the nonlinearity power $ m $, particularly in the supercritical range $ m > m_c = (n-2)_+/n $.
- To provide a stability result that holds for both degenerate ($ m>1 $) and singular ($ m<1 $) cases, including the limiting case $ m=1 $ (heat equation), without requiring $ m \geq 1 $ or $ m \leq 1 $.
- To avoid reliance on advanced tools such as nonlinear semigroup theory, Hölder continuity, or Harnack inequalities, instead using only basic $ L^2 $-based estimates and compactness.
- To extend stability results to initial data that are positive measures of finite mass, such as the Barenblatt solution, which has a Dirac initial trace.
- To provide a direct, elementary proof of convergence in $ L^{1+m} $ norm for both Dirichlet problems on bounded domains and Cauchy problems on $ \mathbb{R}^n $.
Proposed method
- Uses the weak formulation of the equation $ \partial_t u - \Delta u^m = 0 $, where $ u^m $ and $ \nabla u^m $ are in $ L^2 $, enabling $ L^2 $-based energy estimates.
- Applies a compactness principle: locally uniformly bounded sequences of weak solutions admit pointwise a.e. convergent subsequences.
- Employs a test function $ \eta(x,t) = \int_t^T (u^m - u_i^{m_i}) \, ds $ to compare solutions $ u $ and $ u_i $ with different $ m $, leading to energy-type estimates.
- Uses the inequality $ |a-b|^{1+m} \leq c (a^m - b^m)(a-b) $ for $ a,b > 0 $, which holds for $ m > \frac{n-2}{n+2} $, to control the difference in solutions.
- Applies Hölder’s inequality and a pointwise estimate $ |u_i^{m_i} - u_i^m| \leq c(1 + u_i^{m_i+\varepsilon} + u_i^{m+\varepsilon})|m - m_i| $ to bound the difference in nonlinearities.
- Combines Sobolev embedding and energy estimates to obtain uniform $ L^1 $ bounds on $ u_i^{m_i(1+\varepsilon/m_i)(1+1/m)} $, ensuring integrability for small $ \varepsilon $.
Experimental results
Research questions
- RQ1Does the solution to the nonlinear diffusion equation $ \partial_t u - \Delta u^m = 0 $ depend continuously on the exponent $ m $, especially across the degenerate and singular regimes?
- RQ2Can stability of solutions be established without relying on nonlinear semigroup theory or regularity estimates such as Harnack inequalities?
- RQ3Is the convergence of solutions valid when the initial data are positive measures (e.g., Dirac delta), as in the Barenblatt solution?
- RQ4Can the convergence be quantified in terms of the difference $ |m - m_i| $, and what is the rate of convergence in $ L^{1+m} $ norm?
- RQ5Does the stability result extend to the limit $ m \to 1 $, including the case where the limit equation is the classical heat equation?
Key findings
- Solutions to the porous medium and fast diffusion equations converge in $ L^{1+m} $ norm as $ m_i \to m $, with the convergence rate $ \|u - u_i\|_{L^{1+m}(\Omega_T)} \leq c |m - m_i|^{1/m} $ for large $ i $, under the condition $ m > \frac{n-2}{n+2} $.
- The stability result holds for both $ m > 1 $ (degenerate) and $ m < 1 $ (singular) cases, including the limiting case $ m = 1 $, which corresponds to the heat equation.
- The convergence is established for Dirichlet problems on bounded domains and Cauchy problems on $ \mathbb{R}^n $ with initial data being a positive measure of finite mass, such as the Barenblatt solution.
- The Barenblatt solution $ \mathcal{B}_m $ satisfies $ \mathcal{B}_{m_i} \to \mathcal{B}_m $ in $ L^p $ as $ m_i \to m $, a result not previously established in the literature.
- The proof avoids the use of nonlinear semigroup theory, Hölder regularity, or reverse Hölder inequalities, relying only on weak solutions and compactness.
- For $ m \geq 1 $, an alternative proof provides an estimate of the solution difference in terms of $ |m - m_i| $, but this approach is restricted to $ m \geq 1 $ and uses strong monotonicity.
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This review was created by AI and reviewed by human editors.