<p>This manuscript investigates the spherical density of the lower Hewitt–Stromberg measure in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {R}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation>. Also, we establish that if <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(S=(S_1,\ldots ,S_n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <mo>=</mo> <mo stretchy="false">(</mo> <msub> <mi>S</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>…</mo> <mo>,</mo> <msub> <mi>S</mi> <mi>n</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is an iterated function system fulfilling the strong open set condition for some open set <i>U</i>, then <Equation ID="Equ44"> <EquationSource Format="TEX">\(\begin{aligned} \mathcal {U}^\alpha (K_S \cap U(x,r)) \le (2r)^\alpha , \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mrow> <mi mathvariant="script">U</mi> </mrow> <mi>α</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>K</mi> <mi>S</mi> </msub> <mo>∩</mo> <mi>U</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>≤</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mi>α</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>for every open ball <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(U(x,r)\subset U\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>U</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> <mo>⊂</mo> <mi>U</mi> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(x\in K_S\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>∈</mo> <msub> <mi>K</mi> <mi>S</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(r&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>r</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. Employing this estimate, we derive an exact formula for the lower Hewitt–Stromberg measure of self-similar sets. As a consequence, we show that the mapping <Equation ID="Equ45"> <EquationSource Format="TEX">\(\begin{aligned} M_{SSC} \longrightarrow \mathbb {R}: S \longmapsto \mathcal {U}^\alpha (K_S), \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>M</mi> <mrow> <mi mathvariant="italic">SSC</mi> </mrow> </msub> <mo stretchy="false">⟶</mo> <mi mathvariant="double-struck">R</mi> <mo>:</mo> <mi>S</mi> <mo>⟼</mo> <msup> <mrow> <mi mathvariant="script">U</mi> </mrow> <mi>α</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>K</mi> <mi>S</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>is continuous, where <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(M_{SSC}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>M</mi> <mrow> <mi mathvariant="italic">SSC</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> denotes the class of all iterated function systems fulfilling the strong separation condition.</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

An Exact Formula for the Lower Hewitt-Stromberg Measure of Self-Similar Sets and Its Continuity

  • Haythem Zyoudi

摘要

This manuscript investigates the spherical density of the lower Hewitt–Stromberg measure in \(\mathbb {R}^d\) R d . Also, we establish that if \(S=(S_1,\ldots ,S_n)\) S = ( S 1 , , S n ) is an iterated function system fulfilling the strong open set condition for some open set U, then \(\begin{aligned} \mathcal {U}^\alpha (K_S \cap U(x,r)) \le (2r)^\alpha , \end{aligned}\) U α ( K S U ( x , r ) ) ( 2 r ) α , for every open ball \(U(x,r)\subset U\) U ( x , r ) U with \(x\in K_S\) x K S and \(r>0\) r > 0 . Employing this estimate, we derive an exact formula for the lower Hewitt–Stromberg measure of self-similar sets. As a consequence, we show that the mapping \(\begin{aligned} M_{SSC} \longrightarrow \mathbb {R}: S \longmapsto \mathcal {U}^\alpha (K_S), \end{aligned}\) M SSC R : S U α ( K S ) , is continuous, where \(M_{SSC}\) M SSC denotes the class of all iterated function systems fulfilling the strong separation condition.