Search arXiv⌕ Search

arXiv · 2610.25239

An Exact Mass Threshold for Global Existence and Blow-up in Semilinear Anti-de Sitter Equations

Abstract

We study the influence of the mass parameter on global existence and finite-time blow-up for the semilinear anti-de Sitter Klein--Gordon equation \[ ϕ_{tt}-e^{2t}Δϕ+nϕ_t+m^2ϕ=|ϕ|^p \qquad\text{in }[0,\infty)\times\R^d. \] After removing the damping term, we establish $L^2$ energy estimates for the resulting Klein--Gordon equation with constant coefficient in the potential. They imply global existence for arbitrary sufficiently small energy data, without spatial localization, whenever \( m^2>-\frac{d(2n+d)}{4} \quad\text{and}\quad p>1. \) In the remaining mass parameter interval above the structural threshold, an exact change to conformal time reduces the problem to a scale-invariant effective damped wave equation. Exponentially weighted energy estimates then extend global existence to \( -d(n+d) 1. \) In the complementary regime $m^2\le-d(n+d)$, we prove finite-time blow-up for every $p>1$ and for weak solutions with finite speed of propagation arising from nonnegative, nontrivial initial data. We further obtain lifespan estimates that are polynomial at the threshold and logarithmic below it. Thus, $m^2=-d(n+d)$ is the exact structural mass parameter threshold separating the global-existence and blow-up regimes.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Wanderley Nunes do Nascimento, Michael Reissig. 2026-10-18. An Exact Mass Threshold for Global Existence and Blow-up in Semilinear Anti-de Sitter Equations. https://arxiv.org/abs/2610.25239

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

On the dispersive estimates for the discrete Schrödinger equation on a honeycomb lattice

The discrete Schrödinger equation on a two-dimensional honeycomb lattice is a fundamental tight-binding approximation model that describes the propagation of waves on graphene. For free evolution, we first show that the degenerate frequencies of the dispersion relation are completely characterized by three symmetric periodic curves (Theorem 2.1), and that the three curves meet at Dirac points where conical singularities appear (see Figure 2.1). Based on this observation, we prove the $L^1\to L^\infty$ dispersion estimates for the linear flow depending on the frequency localization (Theorem 2.3). Collecting all, we obtain the dispersion estimate with $O(|t|^{-2/3})$ decay as well as Strichartz estimates. As an application, we prove small data scattering for a nonlinear model (Theorem 2.10). The proof of the key dispersion estimates is based on the associated oscillatory integral estimates with degenerate phases and conical singularities at Dirac points. Our proof is direct and uses only elementary methods.

math.AP↗

Well-posedness and Stability of Thermoelastic Suspension Bridges with Cattaneo Heat Conduction: The Role of Viscoelastic Memory

Thermoelastic suspension bridges operate under strong thermo-mechanical coupling, and the classical Fourier law fails to capture the finite speed of thermal propagation observed in low-conductivity materials such as concrete. This paper investigates a suspension bridge model in which the heat flux is governed by the Cattaneo law with relaxation time $τ$, and in which the bridge deck may or may not possess viscoelastic memory. Using operator semigroup theory, we establish well-posedness and derive sharp decay rates for both regimes. For the memoryless system ($δ=0$), we show that the semigroup is polynomially stable with rate $t^{-1/2}$ when the structural parameters satisfy $\frac{ρ_1}κ = \frac{ρ_2}{b}$, and that the rate deteriorates to $t^{-1/4}$ otherwise; moreover, exponential stability fails whenever $χ_0 \neq 0$, or $χ_0 = 0$ and $χ_1 = 0$, where $χ_0$ and $χ_1$ are parameter-dependent coefficients. In sharp contrast, when viscoelastic memory is present ($δ=1$), the semigroup becomes exponentially stable, regardless of the structural parameter ratio. This reveals a regularizing role of viscoelastic memory: it converts polynomial decay into exponential decay and removes the parameter-ratio obstruction. The results provide a theoretical basis for exploiting inherent viscoelasticity in long-span bridges and for optimizing deck parameters in memoryless structures.

math.AP↗