Search arXiv⌕ Search

arXiv · 2610.25278

New Bernstein functions and subordination representations for time-nonlocal evolution equations

Abstract

This paper establishes subordination representations from multi-term time-fractional differential equations to single-term ones, a direction complementary to the previously known subordination from single-term to multi-term equations; combining the two complementary directions also yields subordination representations between two multi-term equations. The crucial step is to prove that certain implicitly defined functions are Bernstein functions. We show that the quotient $\big(\sum_{j=1}^m a_jλ^{α_j}\big)/\big(\sum_{j=1}^m a_jα_jλ^{α_j}\big)$ is a Stieltjes function whenever $0\leqα_1-α_m\leq 1$, and consequently that the inverse function of $λ=\big(\sum_{j=1}^m a_jφ^{α_j}\big)^{1/β}$ is a Bernstein function for every $0<β\leqα_m$. As applications, we obtain subordination representations with a clear probabilistic meaning: from multi-term to single-term time-fractional diffusion-wave equations, between abstract nonlocal-in-time equations with kernels of type $(\mathcal{PC})$ (including equations of tempered stable type), and between nonlocal-in-time telegraph equations. A necessary and sufficient condition for $[(λ+b)^β-b^β]^γ$ to be a Bernstein function also yields a negative result: in general, no such subordination exists from an $α$-stable type dynamics to a tempered $β$-stable one when $α<1$.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Calvin Khor, Cheng-Gang Li. 2026-10-18. New Bernstein functions and subordination representations for time-nonlocal evolution equations. https://arxiv.org/abs/2610.25278

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↗