<p>Let <i>G</i> be a complex semisimple Lie group and <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathfrak {g}\)</EquationSource> </InlineEquation> its Lie algebra. In this paper, we study a special class of cyclic Higgs bundles constructed from a <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {Z}\)</EquationSource> </InlineEquation>-grading <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathfrak {g}= \bigoplus _{j=1-m}^{m-1}\mathfrak {g}_j\)</EquationSource> </InlineEquation> by using the natural representation <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(G_0 \rightarrow {{\,\textrm{GL}\,}}(\mathfrak {g}_1 \oplus \mathfrak {g}_{1-m})\)</EquationSource> </InlineEquation>, where <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(G_0 \leqslant G\)</EquationSource> </InlineEquation> is the connected subgroup corresponding to <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathfrak {g}_0\)</EquationSource> </InlineEquation>. The resulting Higgs pairs include <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(G^\mathbb {R}\)</EquationSource> </InlineEquation>-Higgs bundles for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(G^\mathbb {R}\leqslant G\)</EquationSource> </InlineEquation> a real form of Hermitian type (in the case <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(m=2\)</EquationSource> </InlineEquation>) and fixed points of the <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathbb {C}^*\)</EquationSource> </InlineEquation>-action on <i>G</i>-Higgs bundles (in the case where the Higgs field vanishes along <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mathfrak {g}_{1-m}\)</EquationSource> </InlineEquation>). In both of these situations a topological invariant with interesting properties, known as the Toledo invariant, has been defined and studied in the literature. This paper generalises its definition and properties to the case of arbitrary <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\((G_0,\mathfrak {g}_1 \oplus \mathfrak {g}_{1-m})\)</EquationSource> </InlineEquation>-Higgs pairs, which give rise to families of cyclic Higgs bundles. The results are applied to the example with <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(m=3\)</EquationSource> </InlineEquation> that arises from the theory of quaternion-Kähler symmetric spaces.</p>

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Cyclic Higgs Bundles and the Toledo Invariant

  • Oscar García-Prada,
  • Miguel González

摘要

Let G be a complex semisimple Lie group and \(\mathfrak {g}\) its Lie algebra. In this paper, we study a special class of cyclic Higgs bundles constructed from a \(\mathbb {Z}\) -grading \(\mathfrak {g}= \bigoplus _{j=1-m}^{m-1}\mathfrak {g}_j\) by using the natural representation \(G_0 \rightarrow {{\,\textrm{GL}\,}}(\mathfrak {g}_1 \oplus \mathfrak {g}_{1-m})\) , where \(G_0 \leqslant G\) is the connected subgroup corresponding to \(\mathfrak {g}_0\) . The resulting Higgs pairs include \(G^\mathbb {R}\) -Higgs bundles for \(G^\mathbb {R}\leqslant G\) a real form of Hermitian type (in the case \(m=2\) ) and fixed points of the \(\mathbb {C}^*\) -action on G-Higgs bundles (in the case where the Higgs field vanishes along \(\mathfrak {g}_{1-m}\) ). In both of these situations a topological invariant with interesting properties, known as the Toledo invariant, has been defined and studied in the literature. This paper generalises its definition and properties to the case of arbitrary \((G_0,\mathfrak {g}_1 \oplus \mathfrak {g}_{1-m})\) -Higgs pairs, which give rise to families of cyclic Higgs bundles. The results are applied to the example with \(m=3\) that arises from the theory of quaternion-Kähler symmetric spaces.