<p>In this paper, we first concentrate on the possible values and dense property of entropies for isotropic and anisotropic axial products of subshifts of finite type (SFTs) on <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {N}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">N</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> and <i>d</i>-tree <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation>. We prove that the entropies of isotropic and anisotropic axial products of SFTs on <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {N}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">N</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> are dense in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\([0,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, and the same result also holds for anisotropic axial products of SFTs on <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation>. However, the result is no longer true for isotropic axial products of SFTs on <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation>. Next, motivated by the work of Johnson et al. (Complex Syst 17(3):243, 2007), and Schraudner (Discrete Contin Dyn Syst 26(1):333, 2010), we establish the formulae and structures for entropies of full axial extension shifts on <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {N}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">N</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation>. Combining the aforementioned results with the findings on the surface entropy for multiplicative integer systems (Ban et al. in J Math Phys 64:16, 2023) on <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {N}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">N</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> enables us to estimate the surface entropy for the full axial extension shifts on <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation>. Finally, we extend the results of full axial extension shifts on <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12346_2025_1280_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}_d\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>d</mi> </msub> </math></EquationSource> </InlineEquation> to general trees.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Entropy of Axial Products on \(\mathbb {N}^d\) and Trees

  • Jung-Chao Ban,
  • Wen-Guei Hu,
  • Guan-Yu Lai

摘要

In this paper, we first concentrate on the possible values and dense property of entropies for isotropic and anisotropic axial products of subshifts of finite type (SFTs) on \(\mathbb {N}^d\) N d and d-tree \(\mathcal {T}_d\) T d . We prove that the entropies of isotropic and anisotropic axial products of SFTs on \(\mathbb {N}^d\) N d are dense in \([0,\infty )\) [ 0 , ) , and the same result also holds for anisotropic axial products of SFTs on \(\mathcal {T}_d\) T d . However, the result is no longer true for isotropic axial products of SFTs on \(\mathcal {T}_d\) T d . Next, motivated by the work of Johnson et al. (Complex Syst 17(3):243, 2007), and Schraudner (Discrete Contin Dyn Syst 26(1):333, 2010), we establish the formulae and structures for entropies of full axial extension shifts on \(\mathbb {N}^d\) N d and \(\mathcal {T}_d\) T d . Combining the aforementioned results with the findings on the surface entropy for multiplicative integer systems (Ban et al. in J Math Phys 64:16, 2023) on \(\mathbb {N}^d\) N d enables us to estimate the surface entropy for the full axial extension shifts on \(\mathcal {T}_d\) T d . Finally, we extend the results of full axial extension shifts on \(\mathcal {T}_d\) T d to general trees.