<p>The study of iterated functions is fundamental in complex dynamics. For a holomorphic self-map <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> of the unit disk <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation>, the Denjoy–Wolff theorem (1926) establishes a key convergence property: if <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> is not an elliptic automorphism, then its sequence of iterates, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\((\varphi ^{\circ n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mi>φ</mi> <mrow> <mo>∘</mo> <mi>n</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, converges uniformly on compact subsets to a point <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\tau \in \overline{\mathbb {D}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>τ</mi> <mo>∈</mo> <mover> <mi mathvariant="double-struck">D</mi> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation>, called the Denjoy–Wolff point of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation>. A related question concerns the behavior of these iterates at the boundary. By Fatou’s theorem, all functions <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\varphi ^{\circ n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>φ</mi> <mrow> <mo>∘</mo> <mi>n</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> have non-tangential limits at almost every point on the boundary of the unit disk. We denote these non-tangential limits as <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\((\varphi ^{\circ n})^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>φ</mi> <mrow> <mo>∘</mo> <mi>n</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>. The behavior of the sequence <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(((\varphi ^{\circ n})^*)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>φ</mi> <mrow> <mo>∘</mo> <mi>n</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo>∗</mo> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> depends significantly on whether <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> is an inner function or not. When <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> is an inner function, the behaviour of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(((\varphi ^{\circ n})^*)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>φ</mi> <mrow> <mo>∘</mo> <mi>n</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo>∗</mo> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is well-established and can be found in texts by Aaronson or Doering and Mañé. However, when <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> is not an inner function, the problem was not solved. Previous partial results have been contributed by Bourdon, Matache, and Shapiro; by Poggi-Corradini; and by Contreras, Díaz-Madrigal, and Pommerenke. In this paper, we achieved the final solution: if <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> is not an inner function, then the sequence <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(((\varphi ^{\circ n})^*)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>φ</mi> <mrow> <mo>∘</mo> <mi>n</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> <mo>∗</mo> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> converges to <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>τ</mi> </math></EquationSource> </InlineEquation> for almost every point on <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\partial \mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="double-struck">D</mi> </mrow> </math></EquationSource> </InlineEquation>. Our technique also provides general results on non-autonomous iteration of holomorphic self-maps of the unit disk.</p>

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Convergence on the boundary for iterates of holomorphic self-maps of the unit disk

  • Dimitrios Betsakos,
  • Manuel D. Contreras,
  • Santiago Díaz-Madrigal

摘要

The study of iterated functions is fundamental in complex dynamics. For a holomorphic self-map \(\varphi \) φ of the unit disk \(\mathbb {D}\) D , the Denjoy–Wolff theorem (1926) establishes a key convergence property: if \(\varphi \) φ is not an elliptic automorphism, then its sequence of iterates, \((\varphi ^{\circ n})\) ( φ n ) , converges uniformly on compact subsets to a point \(\tau \in \overline{\mathbb {D}}\) τ D ¯ , called the Denjoy–Wolff point of \(\varphi \) φ . A related question concerns the behavior of these iterates at the boundary. By Fatou’s theorem, all functions \(\varphi ^{\circ n}\) φ n have non-tangential limits at almost every point on the boundary of the unit disk. We denote these non-tangential limits as \((\varphi ^{\circ n})^*\) ( φ n ) . The behavior of the sequence \(((\varphi ^{\circ n})^*)\) ( ( φ n ) ) depends significantly on whether \(\varphi \) φ is an inner function or not. When \(\varphi \) φ is an inner function, the behaviour of \(((\varphi ^{\circ n})^*)\) ( ( φ n ) ) is well-established and can be found in texts by Aaronson or Doering and Mañé. However, when \(\varphi \) φ is not an inner function, the problem was not solved. Previous partial results have been contributed by Bourdon, Matache, and Shapiro; by Poggi-Corradini; and by Contreras, Díaz-Madrigal, and Pommerenke. In this paper, we achieved the final solution: if \(\varphi \) φ is not an inner function, then the sequence \(((\varphi ^{\circ n})^*)\) ( ( φ n ) ) converges to \(\tau \) τ for almost every point on \(\partial \mathbb {D}\) D . Our technique also provides general results on non-autonomous iteration of holomorphic self-maps of the unit disk.