Search arXivSearch

arXiv · 2501.17378

Dimension of diagonal self-affine measures with exponentially separated projections

Abstract

Let $ μ$ be a self-affine measure associated with a diagonal affine iterated function system (IFS) $ Φ= \{ (x_{1}, \ldots, x_{d}) \mapsto ( r_{i, 1}x_{1} + t_{i,1}, \ldots, r_{i,d}x_{d} + t_{i,d}) \}_{i\inΛ} $ on $ \mathbb{R}^{d} $ and a probability vector $ p = (p_{i})_{i\inΛ}$. For $ 1 \leq j \leq d $, denote the $ j $-th the Lyapunov exponent by $ χ_{j} := \sum_{i\inΛ} - p_{i} \log | r_{i,j} |$, and define the IFS induced by $ Φ$ on the $j$-th coordinate as $ Φ_{j} := \{ x \mapsto r_{i,j}x + t_{i,j}\}_{i\inΛ}$. We prove that if $ χ_{j_{1}} \neq χ_{j_{2}} $ for $ 1 \leq j_{1} < j_{2} \leq d $, and $ Φ_{j}$ is exponentially separated for $ 1 \leq j \leq d $, then the dimension of $ μ$ is the minimum of $ d $ and its Lyapunov dimension. This confirms a conjecture of Rapaport by removing the additional assumption that the linear parts of the maps in $ Φ$ are contained in a 1-dimensional subgroup. One of the main ingredients of the proof involves disintegrating $ μ$ into random measures with convolution structure. In the course of the proof, we establish new results on dimension and entropy increase for these random measures.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Zhou Feng. 2025-02-13. Dimension of diagonal self-affine measures with exponentially separated projections. https://arxiv.org/abs/2501.17378

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