English

To Define the Core Entropy for All Polynomials Having a Connected Julia Set

Dynamical Systems 2025-12-30 v4

Abstract

For all polynomials ff with deg(f)2{\rm deg}(f)\ge2 that have a connected filled Julia set KK, we introduce a new quantity hGCE(f)h_{\rm GCE}(f), such that hGCE(fn)=nhGCE(f)h_{\rm GCE}\left(f^n\right)=n\cdot h_{\rm GCE}(f) for all n1n\ge1 and hGCE(f)=hGCE(g)h_{\rm GCE}(f)=h_{\rm GCE}(g) for JJ-equivalent ff and gg. When the coefficients and the critical points of ff are real, hGCE(f)=h(KR,f)h_{\rm GCE}(f)=h(K\cap\mathbb{R},f). When ff is post-critically finite, hGCE(f)h_{\rm GCE}(f) equals the core entropy h(H(f),f)h(\mathcal{H}(f),f), where H(f)\mathcal{H}(f) is the Hubbard tree. For fc(z)=z2+cf_c(z)=z^2+c with cc varying in the Mandelbrot set M\mathcal{M}, the entropy map chGCE(fc)c\mapsto h_{\rm GCE}(f_c) is not continuous. However, its lower envelope hcore:MRh_{\rm core}:\mathcal{M}\rightarrow\mathbb{R} given by hcore(c)=inf{t:  cnc with cnc and t=limnhGCE(fcn)}h_{\rm core}(c)=\inf\left\{t:\ \exists\ c_n\ne c\ \text{with}\ c_n\rightarrow c\ \text{and}\ t=\lim\limits_{n\rightarrow\infty}h_{\rm GCE}\left(f_{c_n}\right)\right\} is continuous over M\mathcal{M} and has three properties. First, every hcore1([0,s])h_{\rm core}^{-1}([0,s]) with s0s\ge0 is connected. In particular, hcore1(0)h_{\rm core}^{-1}(0) coincides with the central molecule. Second, hcore(c)=h(R,fc)h_{\rm core}(c)=h(\mathbb{R},f_c) for c[2,14]c\in[-2,\frac14]. Third, hcore(c)=h(H(fc),fc)h_{\rm core}(c)=h(\mathcal{H}(f_c),f_c) for post-critically finite fcf_c.

Cite

@article{arxiv.2301.12610,
  title  = {To Define the Core Entropy for All Polynomials Having a Connected Julia Set},
  author = {Jun Luo and Bo Tan and Yi Yang and Xiao-Ting Yao},
  journal= {arXiv preprint arXiv:2301.12610},
  year   = {2025}
}

Comments

40 pages, 1 figure

R2 v1 2026-06-28T08:25:49.605Z