Search arXivSearch

arXiv · 2506.23877

Degenerate perturbations of infinite graph-directed iterated function systems

Abstract

We study infinite graph-directed iterated function systems (GIFS) whose underlying graph is not strongly connected and has countably many vertices and edges. In addition to a summability condition for the physical potential, we provide lower and upper estimates of the Hausdorff dimension of the limit set of such GIFS. Bowen type formula is also given under conformal condition and suitable separate conditions. We also introduce perturbed GIFS in which the images of arbitrarily chosen contraction mappings shrink to a single point. In other words, the graph of the perturbed GIFS differs from that of unperturbed GIFS. Assuming suitable continuity condition on contraction mappings, we prove that the Hausdorff dimension of the limit set of the perturbed GIFS converges to that of the unperturbed GIFS, This result generalizes for finite graphs in [T.2019, T.2016] to the infinite graph setting. As applications, we consider a perturbed nonconformal mapping, as well as convergence and non-convergence in the Hausdorff dimension for perturbed complex continued fractions with degeneration.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Haruyoshi Tanaka. 2025-06-30. Degenerate perturbations of infinite graph-directed iterated function systems. https://arxiv.org/abs/2506.23877

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

KEEP EXPLORING

Related papers

Pivoting technique for the circle homeomorphism group

We adapt Gou{ë}zel's pivoting technique to the circle homeomorphism group. As an application, we give different proofs of Gilabert Vio's probabilistic Tits alternative and Malicet's exponential synchronization.

math.DS

Asymmetry of a class of Mellin transforms

We introduce the quantity $μ_η$, defined for every complex $s$ in the critical strip, as a transformation of the Mellin transform associated to the functions $η$. We establish a sufficient condition on $η$ under which $μ_η(s)$ and $μ_η(1-s)$ cannot both vanish outside the critical line. An application is given to the case in which $η$ is the fractional part function, and the zeros of $μ_η$ coincide with the zeros of the Riemann zeta function.

math.DS

Infinite Set of Resonances in the Linear Damped Oscillator Subject to Harmonic Forcing with Non-standard Frequency Modulation

It is shown that harmonic signals incorporating a type of weak non-standard frequency modulation (wNSFM) have interesting spectral properties, namely, time-dependent bandwidths that become increasingly broader with increasing time. As such, they represent a class of signals with frequency-time coupling in their spectra. Specifically, the weakly damped oscillator exhibits always two transient resonance captures involving two distinct harmonics possessing relatively high amplitudes over finite time intervals, while the overall response decays as $~t^{-1/2}$ as $t\rightarrow\infty$. Considering the undamped oscillator, it possesses two types of resonances, referred to as simple and non-simple resonances. Simple resonances correspond to finite-amplitude steady-state responses caused by two sustained resonance captures, in the form of two distinct modulated quasi-periodic responses, which, however are "activated" at different time instances. The necessary and sufficient conditions for non-simple resonances are given in the form of a theorem which predicts the existence of resonant harmonics and specifies the special phase conditions that the resonant harmonics must satisfy for constructive interference; the resulting undamped non-simple resonance grows unboundedly as $~t^{-1/2}$ as $t\rightarrow\infty$, in contrast to the classical resonance growth of the linear resonator with unmodulated harmonic excitation whose response grows as $~t$ as $t\rightarrow\infty$. These resonant responses are persistent to changes in the parameters of the wNSFM. Our results reveal interesting infinite sets of resonances in linear SDOF resonators under frequency-modulated excitations.

math.DS