<p>Let <i>M</i> be a compact symplectic manifold carrying a Hamiltonian <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(S^1\)</EquationSource> </InlineEquation>-action with momentum map <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({ \mathrm J}:M \rightarrow {\mathbb R}\)</EquationSource> </InlineEquation> and consider the corresponding symplectic quotient <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({\mathscr {M}}_0:={ \mathrm J}^{-1}(0)/S^1\)</EquationSource> </InlineEquation>. We extend Sjamaar’s complex of differential forms on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({\mathscr {M}}_0\)</EquationSource> </InlineEquation>, whose cohomology is isomorphic to the singular or Čech cohomology <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H^{*}({\mathscr {M}}_0)\)</EquationSource> </InlineEquation> of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({\mathscr {M}}_0\)</EquationSource> </InlineEquation> with real coefficients, to a complex of differential forms on <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({\mathscr {M}}_0\)</EquationSource> </InlineEquation> associated with a partial desingularization <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\widetilde{{\mathscr {M}}_0}\)</EquationSource> </InlineEquation> of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({\mathscr {M}}_0\)</EquationSource> </InlineEquation>, which we call resolution differential forms. The cohomology of that complex turns out to be isomorphic to the de Rham cohomology <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(H^{*}(\widetilde{{\mathscr {M}}_0})\)</EquationSource> </InlineEquation> of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\widetilde{{\mathscr {M}}_0}\)</EquationSource> </InlineEquation>. Based on this, we derive a long exact sequence involving both <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(H^{*}({\mathscr {M}}_0)\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(H^{*}(\widetilde{{\mathscr {M}}_0})\)</EquationSource> </InlineEquation> and give conditions for its splitting. We then define a Kirwan map <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathcal {K}:H_{S^1}^{*}(M) \rightarrow H^{*}(\widetilde{{\mathscr {M}}_0})\)</EquationSource> </InlineEquation> from the equivariant cohomology <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(H_{S^1}^{*}(M)\)</EquationSource> </InlineEquation> of <i>M</i> to <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(H^{*}(\widetilde{{\mathscr {M}}_0})\)</EquationSource> </InlineEquation> and show that its image contains the image of <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(H^{*}({\mathscr {M}}_0)\)</EquationSource> </InlineEquation> in <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(H^{*}(\widetilde{{\mathscr {M}}_0})\)</EquationSource> </InlineEquation> under the natural inclusion. Combining both results in the case that all fixed point components of <i>M</i> have vanishing odd cohomology we obtain a surjection <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\check{\kappa }:H^\text {ev}_{S^1}(M) \rightarrow H^\text {ev}({\mathscr {M}}_0)\)</EquationSource> </InlineEquation> in even degrees, while already simple examples show that a similar surjection in odd degrees does not exist in general. As an interesting class of examples we study abelian polygon spaces.</p>

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Singular Cohomology of Symplectic Quotients by Circle Actions and Kirwan Surjectivity

  • Benjamin Delarue,
  • Pablo Ramacher,
  • Maximilian Schmitt

摘要

Let M be a compact symplectic manifold carrying a Hamiltonian \(S^1\) -action with momentum map \({ \mathrm J}:M \rightarrow {\mathbb R}\) and consider the corresponding symplectic quotient \({\mathscr {M}}_0:={ \mathrm J}^{-1}(0)/S^1\) . We extend Sjamaar’s complex of differential forms on \({\mathscr {M}}_0\) , whose cohomology is isomorphic to the singular or Čech cohomology \(H^{*}({\mathscr {M}}_0)\) of \({\mathscr {M}}_0\) with real coefficients, to a complex of differential forms on \({\mathscr {M}}_0\) associated with a partial desingularization \(\widetilde{{\mathscr {M}}_0}\) of \({\mathscr {M}}_0\) , which we call resolution differential forms. The cohomology of that complex turns out to be isomorphic to the de Rham cohomology \(H^{*}(\widetilde{{\mathscr {M}}_0})\) of \(\widetilde{{\mathscr {M}}_0}\) . Based on this, we derive a long exact sequence involving both \(H^{*}({\mathscr {M}}_0)\) and \(H^{*}(\widetilde{{\mathscr {M}}_0})\) and give conditions for its splitting. We then define a Kirwan map \(\mathcal {K}:H_{S^1}^{*}(M) \rightarrow H^{*}(\widetilde{{\mathscr {M}}_0})\) from the equivariant cohomology \(H_{S^1}^{*}(M)\) of M to \(H^{*}(\widetilde{{\mathscr {M}}_0})\) and show that its image contains the image of \(H^{*}({\mathscr {M}}_0)\) in \(H^{*}(\widetilde{{\mathscr {M}}_0})\) under the natural inclusion. Combining both results in the case that all fixed point components of M have vanishing odd cohomology we obtain a surjection \(\check{\kappa }:H^\text {ev}_{S^1}(M) \rightarrow H^\text {ev}({\mathscr {M}}_0)\) in even degrees, while already simple examples show that a similar surjection in odd degrees does not exist in general. As an interesting class of examples we study abelian polygon spaces.