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On the existence of non-negative weak solutions for $1D$ fourth order equations of gradient flow type

Stefanos Georgiadis, Stefano Spirito

TL;DR

This work studies a family of 1D fourth-order gradient-flow PDEs derived from the Korteweg energy, unifying models such as the Quantum-Drift-Diffusion and Thin-Film equations. It proves the global-in-time existence of non-negative weak solutions for all $β > -3$ under mild initial-data assumptions, without requiring an a priori bound on the energy exponent. The core method combines gradient-flow energy and entropy dissipations with an ε-regularized approximating system that preserves a skew-adjoint structure to avoid derivative loss, enabling uniform bounds and compactness. A careful convergence analysis (via Aubin–Lions and strong/weak convergences of density powers) yields a limit that satisfies the weak formulation and energy/entropy inequalities, establishing global solvability in one dimension. The results extend the one-dimensional theory beyond previously known ranges and support broader applicability of these gradient-flow models in capillarity, quantum diffusion, and related diffusion processes.

Abstract

In this paper, we consider a family of one-dimensional fourth order evolution equations arising as gradient flows of the Korteweg energy, i.e. the $L^2$-norm of the first derivative of some power of the density. This family of equations generalizes the Quantum-Drift-Diffusion equation and the Thin-Film equation. We prove the global-in-time existence of {\em non-negative} weak solutions without requiring any upper bound on the exponent of the power of the density in the energy.

On the existence of non-negative weak solutions for $1D$ fourth order equations of gradient flow type

TL;DR

This work studies a family of 1D fourth-order gradient-flow PDEs derived from the Korteweg energy, unifying models such as the Quantum-Drift-Diffusion and Thin-Film equations. It proves the global-in-time existence of non-negative weak solutions for all under mild initial-data assumptions, without requiring an a priori bound on the energy exponent. The core method combines gradient-flow energy and entropy dissipations with an ε-regularized approximating system that preserves a skew-adjoint structure to avoid derivative loss, enabling uniform bounds and compactness. A careful convergence analysis (via Aubin–Lions and strong/weak convergences of density powers) yields a limit that satisfies the weak formulation and energy/entropy inequalities, establishing global solvability in one dimension. The results extend the one-dimensional theory beyond previously known ranges and support broader applicability of these gradient-flow models in capillarity, quantum diffusion, and related diffusion processes.

Abstract

In this paper, we consider a family of one-dimensional fourth order evolution equations arising as gradient flows of the Korteweg energy, i.e. the -norm of the first derivative of some power of the density. This family of equations generalizes the Quantum-Drift-Diffusion equation and the Thin-Film equation. We prove the global-in-time existence of {\em non-negative} weak solutions without requiring any upper bound on the exponent of the power of the density in the energy.

Paper Structure

This paper contains 13 sections, 9 theorems, 171 equations.

Key Result

Theorem 1.1

Assume that $\beta>-3$. Let $\rho^0\in L^{1}(\mathbb{T})$ be such that $\rho^0\geq 0$ if $\beta>-2$, and $m^0:=\min_{x\in\mathbb{T}}\rho^0(x)>0$ if $-3<\beta\leq-2$. Assume also that Then, there exists a global-in-time non-negative weak solution of eq:gfb-eq:gfgid, in the sense of Definition def:ws.

Theorems & Definitions (22)

  • Theorem 1.1
  • Remark 1
  • Definition 2.1
  • Remark 2
  • Proposition 3.1
  • proof
  • Lemma 3.2
  • Remark 3
  • proof
  • Theorem 4.1
  • ...and 12 more