<p>Ahlfors’ Second Fundamental Theorem for the simply connected surfaces over the Riemann sphere <i>S</i> states that for any set <i>E</i><sub><i>q</i></sub> of distinct <i>q</i> points on <i>S</i> with <i>q</i> ≥ 3, there exists a constant <i>h</i> = <i>h</i>(<i>E</i><sub><i>q</i></sub>), such that for any covering surface <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Sigma=(f, \ {\overline U})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mi mathvariant="normal">Σ</mi> <mo>=</mo> <mo stretchy="false">(</mo> <mi>f</mi> <mo>,</mo> <mrow> <mover> <mi>U</mi> <mo accent="false">¯</mo> </mover> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation>, one has <Equation ID="Equa"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_Equa.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="279" /> </MediaObject> <EquationSource Format="TEX">\((q-2) \ A(\Sigma) \leq 4{\pi}{\overline n}(\Sigma, \ E_{q})+hL(\partial\Sigma),\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo stretchy="false">(</mo> <mi>q</mi> <mo>−</mo> <mn>2</mn> <mo stretchy="false">)</mo> <mi>A</mi> <mo stretchy="false">(</mo> <mi mathvariant="normal">Σ</mi> <mo stretchy="false">)</mo> <mo>≤</mo> <mn>4</mn> <mrow> <mi>π</mi> </mrow> <mrow> <mover> <mi>n</mi> <mo accent="false">¯</mo> </mover> </mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Σ</mi> <mo>,</mo> <msub> <mi>E</mi> <mrow> <mi>q</mi> </mrow> </msub> <mo stretchy="false">)</mo> <mo>+</mo> <mi>h</mi> <mi>L</mi> <mo stretchy="false">(</mo> <mi mathvariant="normal">∂</mi> <mi mathvariant="normal">Σ</mi> <mo stretchy="false">)</mo> <mo>,</mo> </math></EquationSource> </Equation> where <i>U</i> is a Jordan domain in <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="97" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb C}, f : {\overline U} \rightarrow S\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> </mrow> <mo>,</mo> <mi>f</mi> <mo>:</mo> <mrow> <mover> <mi>U</mi> <mo accent="false">¯</mo> </mover> </mrow> <mo stretchy="false">→</mo> <mi>S</mi> </math></EquationSource> </InlineEquation> is an orientation-preserving, continuous, open and finite-to-one mapping, <i>A</i>(Σ) is the spherical area of Σ, <i>L</i>(<i>∂</i>Σ) is the spherical length of the boundary of Σ and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="205" /> </InlineMediaObject> <EquationSource Format="TEX">\({\overline n}(\Sigma, \ E_{q})=\#[f^{-1}(E_{q}) \ \cap U]\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mi>n</mi> <mo accent="false">¯</mo> </mover> </mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Σ</mi> <mo>,</mo> <msub> <mi>E</mi> <mrow> <mi>q</mi> </mrow> </msub> <mo stretchy="false">)</mo> <mo>=</mo> <mi mathvariant="normal">#</mi> <mo stretchy="false">[</mo> <msup> <mi>f</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> <mo stretchy="false">(</mo> <msub> <mi>E</mi> <mrow> <mi>q</mi> </mrow> </msub> <mo stretchy="false">)</mo> <mo>∩</mo> <mi>U</mi> <mo stretchy="false">]</mo> </math></EquationSource> </InlineEquation> means the cardinality of the set <i>f</i><sup>−1</sup> (<i>E</i><sub><i>q</i></sub>) ∩ <i>U</i>. We denote by <b>F</b> the space of all simply covering surfaces over the sphere, the above pairs <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\((f, \ {\overline U})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo stretchy="false">(</mo> <mi>f</mi> <mo>,</mo> <mrow> <mover> <mi>U</mi> <mo accent="false">¯</mo> </mover> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation>, and write <b>F</b> (<i>L</i>) = {Σ ∈ <b>F</b>: <i>L</i>(<i>∂</i>Σ) ≤ <i>L</i>}. In a preprint by the third author Zhang of this paper, the precised bound of <i>h</i> is identified (see arXiv.2307.04623). The first key step of Zhang’s method is to prove the existence of extremal surfaces of the subspace <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\({\cal F}(L, \ m)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="script">F</mi> </mrow> <mo stretchy="false">(</mo> <mi>L</mi> <mo>,</mo> <mi>m</mi> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> of <b>F</b> (<i>L</i>), and Zhang asserted without proof in that paper that the extremal surface of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\({\cal F}(L, \ m)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="script">F</mi> </mrow> <mo stretchy="false">(</mo> <mi>L</mi> <mo>,</mo> <mi>m</mi> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> can be found in the smaller subspace <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="72" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\cal F}_{r}}(L, \ m)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mrow> <mi mathvariant="script">F</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> <mo stretchy="false">(</mo> <mi>L</mi> <mo>,</mo> <mi>m</mi> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> such that the defining function <i>f</i> of each surface of the form <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq8.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\((f, {\overline \Delta})\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo stretchy="false">(</mo> <mi>f</mi> <mo>,</mo> <mrow> <mover> <mi mathvariant="normal">Δ</mi> <mo accent="false">¯</mo> </mover> </mrow> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11464_2023_86_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="72" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\cal F}_{r}}(L, \ m)\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mrow> <mi mathvariant="script">F</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> <mo stretchy="false">(</mo> <mi>L</mi> <mo>,</mo> <mi>m</mi> <mo stretchy="false">)</mo> </math></EquationSource> </InlineEquation> has no branch value outside <i>E</i><sub><i>q</i></sub>. In this paper, we prove this assertion.</p>

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Movement of Branch Points in Ahlfors’ Theory of Covering Surfaces

  • Yunling Chen,
  • Tianrun Lin,
  • Guangyuan Zhang

摘要

Ahlfors’ Second Fundamental Theorem for the simply connected surfaces over the Riemann sphere S states that for any set Eq of distinct q points on S with q ≥ 3, there exists a constant h = h(Eq), such that for any covering surface \(\Sigma=(f, \ {\overline U})\) Σ = ( f , U ¯ ) , one has \((q-2) \ A(\Sigma) \leq 4{\pi}{\overline n}(\Sigma, \ E_{q})+hL(\partial\Sigma),\) ( q 2 ) A ( Σ ) 4 π n ¯ ( Σ , E q ) + h L ( Σ ) , where U is a Jordan domain in \({\mathbb C}, f : {\overline U} \rightarrow S\) C , f : U ¯ S is an orientation-preserving, continuous, open and finite-to-one mapping, A(Σ) is the spherical area of Σ, L(Σ) is the spherical length of the boundary of Σ and \({\overline n}(\Sigma, \ E_{q})=\#[f^{-1}(E_{q}) \ \cap U]\) n ¯ ( Σ , E q ) = # [ f 1 ( E q ) U ] means the cardinality of the set f−1 (Eq) ∩ U. We denote by F the space of all simply covering surfaces over the sphere, the above pairs \((f, \ {\overline U})\) ( f , U ¯ ) , and write F (L) = {Σ ∈ F: L(Σ) ≤ L}. In a preprint by the third author Zhang of this paper, the precised bound of h is identified (see arXiv.2307.04623). The first key step of Zhang’s method is to prove the existence of extremal surfaces of the subspace \({\cal F}(L, \ m)\) F ( L , m ) of F (L), and Zhang asserted without proof in that paper that the extremal surface of \({\cal F}(L, \ m)\) F ( L , m ) can be found in the smaller subspace \({{\cal F}_{r}}(L, \ m)\) F r ( L , m ) such that the defining function f of each surface of the form \((f, {\overline \Delta})\) ( f , Δ ¯ ) in \({{\cal F}_{r}}(L, \ m)\) F r ( L , m ) has no branch value outside Eq. In this paper, we prove this assertion.