<p>The non-abelian Hodge correspondence is a real analytic map between the moduli space of stable Higgs bundles and the deRham moduli space of irreducible flat connections mediated by solutions to the self-duality equations. In this paper we construct self-duality solutions for strongly parabolic <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {sl}(2,{{\mathbb {C}}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">sl</mi> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> Higgs fields on a 4-punctured sphere with parabolic weights <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(t \sim 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∼</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> using complex analytic methods. We identify the rescaled limit hyper-Kähler moduli space <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {M}}_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">M</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> at <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(t=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> to be the completion of the nilpotent orbit in <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {sl}(2, {{\mathbb {C}}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">sl</mi> <mo stretchy="false">(</mo> <mn>2</mn> <mo>,</mo> <mi mathvariant="double-struck">C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> modulo a <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="57" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathbb {Z}}}_2\times {{\mathbb {Z}}}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> <mo>×</mo> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> action, equipped with the Eguchi–Hanson metric. Our methods and computations are based on the twistor approach to the self-duality equations using Deligne and Simpson’s <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>-connections interpretation. By construction we can compute the Taylor expansions of the holomorphic symplectic form <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq8.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varpi _t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ϖ</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {M}}_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">M</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> at <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(t=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> which turn out to have closed form expressions in terms of multiple polylogarithms (MPLs). The geometric properties of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3165_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {M}}_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">M</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> lead to some identities of certain MPLs which we believe deserve further investigations.</p>

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Loop group methods for the non-abelian Hodge correspondence on a 4-punctured sphere

  • Lynn Heller,
  • Sebastian Heller,
  • Martin Traizet

摘要

The non-abelian Hodge correspondence is a real analytic map between the moduli space of stable Higgs bundles and the deRham moduli space of irreducible flat connections mediated by solutions to the self-duality equations. In this paper we construct self-duality solutions for strongly parabolic \(\mathfrak {sl}(2,{{\mathbb {C}}})\) sl ( 2 , C ) Higgs fields on a 4-punctured sphere with parabolic weights \(t \sim 0\) t 0 using complex analytic methods. We identify the rescaled limit hyper-Kähler moduli space \({\mathcal {M}}_t\) M t at \(t=0\) t = 0 to be the completion of the nilpotent orbit in \(\mathfrak {sl}(2, {{\mathbb {C}}})\) sl ( 2 , C ) modulo a \({{\mathbb {Z}}}_2\times {{\mathbb {Z}}}_2\) Z 2 × Z 2 action, equipped with the Eguchi–Hanson metric. Our methods and computations are based on the twistor approach to the self-duality equations using Deligne and Simpson’s \(\lambda \) λ -connections interpretation. By construction we can compute the Taylor expansions of the holomorphic symplectic form \(\varpi _t\) ϖ t on \({\mathcal {M}}_t\) M t at \(t=0\) t = 0 which turn out to have closed form expressions in terms of multiple polylogarithms (MPLs). The geometric properties of \({\mathcal {M}}_t\) M t lead to some identities of certain MPLs which we believe deserve further investigations.