SearcharxivSearch

arXiv · 2507.16072

Asymptotic consensus with transmission and reaction delay: an overview

Abstract

The aim of this paper is to provide a systematic overview of results on asymptotic consensus for the Hegselmann-Krause-type model with delay and discuss the corresponding analytical tools. We explain that two types (sources) of delay - transmission and reaction - are justifiable from the modeling point of view. We consider both classical and normalized communication weights. Studying a toy model with two agents only, we develop an intuitive insight into what type of dynamics we can expect from the systems. In particular, we stress that with transmission-type delay, asymptotic consensus can be reached with any length of the delay (i.e., without smallness assumptions). In contrast, the systems with reaction-type delay can only reach asymptotic consensus if the delay is sufficiently small. We formulate four theorems that establish asymptotic consensus in the following scenarios: (1) transmission-type delay with classical communication weights, (2) transmission-type delay with normalized communication weights, (3) reaction-type delay with symmetric communication weights, (4) reaction-type delay with non-symmetric communication weights. We explain how the methods of proof depend on the particular scenario: direct estimates for (1), convexity arguments for (2), Lyapunov functional for (3) and generalized Gronwall-Halanay inequality for (4).

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Jan Haskovec. 2025-07-21. Asymptotic consensus with transmission and reaction delay: an overview. https://arxiv.org/abs/2507.16072

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

KEEP EXPLORING

Related papers

Admissible Fourier Lengths, KAM Reducibility, and Spectral Applications

We develop a perturbative KAM reducibility theory for one-frequency $\mathrm{SL}(2,\mathbb{R})$ cocycles based on an admissible Fourier length $\ell$. The regularity relevant to the iteration is measured by positive adapted Fourier width rather than ordinary smoothness in the Euclidean length $|n|$. The same length governs Fourier decay, truncation and resonance scales, and the arithmetic condition controlling the small divisors. This framework contains the classical analytic and Gevrey settings, while non-monotone choices of $\ell$ allow classical nowhere differentiable Weierstrass-type perturbations and continuous perturbations outside every positive H\"older class. As spectral applications, we obtain purely absolutely continuous spectrum for every phase and $1/2$-H\"older continuity of the integrated density of states for the associated quasiperiodic Schr\"odinger operators. The Aubry dual has pure point spectrum for Lebesgue almost every dual phase, with eigenfunctions exponentially localized in the metric induced by $\ell$. We also construct nowhere differentiable quasiperiodic potentials with purely absolutely continuous Cantor spectrum.

math.DS

Dynamics inside the attracting basins of some skew products

Polynomial skew products in $\mathbb{C}^2$ are maps of the form $F(z,w)=(P(z),Q(z,w))$, where $P$ and $Q$ are polynomials. Their local dynamics have been widely investigated. In this paper, we study the global dynamics inside Fatou components of some skew products. We consider all the inverse images in a Fatou component of a given point and use the Kobayashi metric to measure the distance between points. In the cases we consider, there are always arbitrarily large Kobayashi balls in the complement of these inverse sets.

math.DS

Ergodicity of dynamical systems without uniqueness of orbits

Recently, there has been considerable interest in the study of non-deterministic dynamical systems. To analyze the chaotic behavior of such systems from a measure-theoretic viewpoint, it is desirable to consider ergodicity. However, the classical definition of ergodicity involves invariant sets, whose definition is not unique for non-deterministic dynamical systems. Thus, we are led to the question of which invariance yields an interesting definition of ergodicity. Here, we propose a definition based on the strong backward invariance and show that analogs of classical results hold. We also consider implications of the Birkhoff ergodic theorem for systems without uniqueness of orbits.

math.DS