<p>The work of Bryant [<CitationRef CitationID="CR7">7</CitationRef>] revealed striking analogies between constant mean curvature (CMC) 1-immersions of surfaces into the hyperbolic space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {H}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">H</mi> </mrow> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation> (Bryant surfaces) and minimal immersions into the euclidean space <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {E}^3.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="double-struck">E</mi> </mrow> <mn>3</mn> </msup> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> Ever since, the role of (CMC) 1-immersions in hyperbolic geometry has been widely explored, see e.g. [<CitationRef CitationID="CR44">44</CitationRef>] and references therein. In account of [<CitationRef CitationID="CR16">16</CitationRef>, <CitationRef CitationID="CR53">53</CitationRef>] and after [<CitationRef CitationID="CR48">48</CitationRef>], for a given surface <i>S</i> (closed, orientable and of genus <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathfrak {g}\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">g</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) here we pursue the existence and uniqueness of (CMC) 1-immersions of <i>S</i> into hyperbolic 3-manifolds. It has been shown in [<CitationRef CitationID="CR22">22</CitationRef>] that, for <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\vert c \vert &lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mi>c</mi> <mo stretchy="false">|</mo> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, the moduli space of (CMC) <i>c</i>-immersions of <i>S</i> into hyperbolic 3-manifolds can be parametrised by elements of the tangent bundle of the Teichmüller space of the surface <i>S</i>. In turn in [<CitationRef CitationID="CR48">48</CitationRef>] it was pointed out that (CMC) 1-immersions enter as "critical" objects, in the sense that they can be attained only as limits of (CMC) <i>c</i>-immersions, as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(|c| \rightarrow 1^-.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mi>c</mi> <mo stretchy="false">|</mo> </mrow> <mo stretchy="false">→</mo> <msup> <mn>1</mn> <mo>-</mo> </msup> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> However, the passage to the limit can be prevented by possible blow-up phenomena, and at the limit (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(|c| \rightarrow 1^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mi>c</mi> <mo stretchy="false">|</mo> </mrow> <mo stretchy="false">→</mo> <msup> <mn>1</mn> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>) we could end up at best with an immersed surface having conical singularities supported at finitely many points (the blow-up points). If the genus <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathfrak {g}=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">g</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> then blow up can occur at a single point, and in [<CitationRef CitationID="CR48">48</CitationRef>] it was shown how it could be prevented and the passage to the limit ensured in terms of the image <i>Z</i> of Kodaira map given in (<InternalRef RefID="Equ48">2.30</InternalRef>). In this note we show that actually blow-up can occur only at one of the six Weierstrass points of the surface. Thus, in Theorem <InternalRef RefID="FPar3">1</InternalRef> and Theorem <InternalRef RefID="FPar17">4</InternalRef> we establish existence and uniqueness results under a sufficient "compactness" condition, which in fact turns out to be also necessary, as shown in [<CitationRef CitationID="CR51">51</CitationRef>]. In addition we analyze the case of higher genus, where multiple (up to <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\mathfrak {g}- 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">g</mi> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) blow-up points can occur. In this case, for any <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(1 \le \nu \le \mathfrak {g}- 1,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>≤</mo> <mi>ν</mi> <mo>≤</mo> <mi mathvariant="fraktur">g</mi> <mo>-</mo> <mn>1</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> we identify in the <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\nu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ν</mi> </math></EquationSource> </InlineEquation>-secant variety of <i>Z</i> the appropriate replacement of <i>Z</i> (relative to <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\nu =1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>), see Proposition <InternalRef RefID="FPar11">2.1</InternalRef>. Moreover, in Theorem <InternalRef RefID="FPar15">3</InternalRef> we improve in a substantial way the asymptotic analysis of [<CitationRef CitationID="CR48">48</CitationRef>], which concerns only the case of "blow-up" with minimal mass. As a consequence, we cover the case of genus <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mathfrak {g}=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">g</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> (see Theorem <InternalRef RefID="FPar18">5</InternalRef>), and provide relevant contributions for arbitrary genus.</p>

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On constant mean curvature 1-immersions of surfaces into hyperbolic 3-manifolds.

  • Gabriella Tarantello,
  • Stefano Trapani

摘要

The work of Bryant [7] revealed striking analogies between constant mean curvature (CMC) 1-immersions of surfaces into the hyperbolic space \(\mathbb {H}^3\) H 3 (Bryant surfaces) and minimal immersions into the euclidean space \(\mathbb {E}^3.\) E 3 . Ever since, the role of (CMC) 1-immersions in hyperbolic geometry has been widely explored, see e.g. [44] and references therein. In account of [16, 53] and after [48], for a given surface S (closed, orientable and of genus \(\mathfrak {g}\ge 2\) g 2 ) here we pursue the existence and uniqueness of (CMC) 1-immersions of S into hyperbolic 3-manifolds. It has been shown in [22] that, for \(\vert c \vert <1\) | c | < 1 , the moduli space of (CMC) c-immersions of S into hyperbolic 3-manifolds can be parametrised by elements of the tangent bundle of the Teichmüller space of the surface S. In turn in [48] it was pointed out that (CMC) 1-immersions enter as "critical" objects, in the sense that they can be attained only as limits of (CMC) c-immersions, as \(|c| \rightarrow 1^-.\) | c | 1 - . However, the passage to the limit can be prevented by possible blow-up phenomena, and at the limit ( \(|c| \rightarrow 1^-\) | c | 1 - ) we could end up at best with an immersed surface having conical singularities supported at finitely many points (the blow-up points). If the genus \(\mathfrak {g}=2\) g = 2 then blow up can occur at a single point, and in [48] it was shown how it could be prevented and the passage to the limit ensured in terms of the image Z of Kodaira map given in (2.30). In this note we show that actually blow-up can occur only at one of the six Weierstrass points of the surface. Thus, in Theorem 1 and Theorem 4 we establish existence and uniqueness results under a sufficient "compactness" condition, which in fact turns out to be also necessary, as shown in [51]. In addition we analyze the case of higher genus, where multiple (up to \(\mathfrak {g}- 1\) g - 1 ) blow-up points can occur. In this case, for any \(1 \le \nu \le \mathfrak {g}- 1,\) 1 ν g - 1 , we identify in the \(\nu \) ν -secant variety of Z the appropriate replacement of Z (relative to \(\nu =1\) ν = 1 ), see Proposition 2.1. Moreover, in Theorem 3 we improve in a substantial way the asymptotic analysis of [48], which concerns only the case of "blow-up" with minimal mass. As a consequence, we cover the case of genus \(\mathfrak {g}=3\) g = 3 (see Theorem 5), and provide relevant contributions for arbitrary genus.