Oct 2026· Studies in applied mathematics (Cambridge)· Vol 157· 0 citations· 22 references
Abstract
In this paper, we study an autonomous conformable logistic dynamic equation in proportional conformable calculus on timescales. A reciprocal transformation reduces the nonlinear problem to a mixed first‐order conformable equation and yields an exact representation, including the constant‐coefficient solution with effective carrying capacity Kα=k(1−κ1/r)$K_{\alpha }=k(1-\kappa _1/r)$ . Under the positivity condition Dα(t)=κ0+μ(t)(r−κ1)>0$\mathcal {D}_{\alpha }(t)=\kappa _0+\mu (t)(r-\kappa _1)>0$ , positive solutions are global and forward invariant. According to the relation between r$r$ and κ1$\kappa _1$ , solutions converge to a positive equilibrium, exhibit algebraic extinction in the critical case, or decay exponentially. For the standard proportional choice, the critical order is α∗=1−r$\alpha ^{*}=1-r$ . We also establish conformable‐exponential comparison and conditional Hyers–Ulam stability results. In the standard autonomous case, the equation can be rewritten as a delta logistic model with effective growth and removal coefficients, clarifying how the conformable order controls their balance. The critical order is proved to be a transcritical bifurcation value for constant graininess and for the associated period map on periodic or forward‐periodic timescales. The conditional Hyers–Ulam stability result is formulated through explicit initial‐state and defect thresholds without requiring bounded graininess. The theory is further illustrated on several discrete, hybrid, and Cantor‐type timescales.
In this paper, we determine the propagation rates of the Fisher-KPP equation with free boundaries and fractional diffusion $(-\Delta)^s$ $(0<s<1)$, which was considered in \cite{CDN26} as a model for species spreading, where the density function $u(t,x)$ satisfies the fractional Fisher-KPP equation $u_t+(-\Delta)^su=f(...
We study quasilinear symmetrizable partially dissipative hyperbolic systems with non-autonomous relaxation coefficients in $\mathbb{R}^d$ ($d\geq1$). The existence of global strong solutions is established in a critical regularity setting for systems satisfying the so-called Shizuta-Kawashima (SK) and entropy condition...
We introduce a notion of viscosity solution for Hamilton--Jacobi--Bellman (HJB) equations with distributional drift, based on paracontrolled test functions and related through a Zvonkin transformation to classical viscosity theory. The equations considered are of the form \[ \left(\partial_t+\frac12\Delta+b\cdot\nabla\...
Dirk Becherer, Nicolas Perkowski, Yu-Chen Sun et al.· 0 citations
We study an accelerated Langevin equation in which the classical overdamped Langevin drift is supplemented by a nonlocal gradient velocity determined through a target-weighted Poisson equation. The target $p$ is only assumed to be strictly positive and need not be normalized. Writing the dynamics in terms of $\omega=\l...
Zi-Yue Cai, Wei-Ye Gan, Bo-Rui Miao et al.· 0 citations
We explore the inverse problem of determining the reaction coefficient $q(x',t)$ in the time-fractional diffusion equation ${}^CD_t u-Lu+q(x',t)u=f$ in $\mathbb{R}^n\times(0,T]$, $x=(x',x_n)$, $0<\alpha<1$, from the trace of the solution on the hyperplane $\{x_n=0\}$. Here ${}^CD_t$ is the Gerasimov--Caputo derivative...
We study the master equation $ (\partial_t -\Delta)^{s} u(x,t) = R(|x|)f(u(x,t))\quad\mbox{in}\ \mathbb{R}^n\times\mathbb{R}, $ where $s\in(0,1)$, $R$ is positive and strictly decreasing in the radial variable, and $f$ is positive, locally Lipschitz, and satisfies $f'(0)<0$. Existing symmetry results for this operator...
Ya-Hui Niu· 0 citations
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