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A generalization of Steinberg theory and an exotic moment map

Lucas Fresse, Kyo Nishiyama

Abstract

For a reductive group $G$, Steinberg established a map from the Weyl group to the set of nilpotent $G$-orbits by using moment maps on double flag varieties. In particular, in the case of the general linear group, it provides a geometric interpretation of the Robinson-Schensted correspondence between permutations and pairs of standard tableaux of the same shape. We extend Steinberg's approach to the case of a symmetric pair $(G,K)$ to obtain two different maps, namely a \emph{generalized Steinberg map} and an \emph{exotic moment map}. Although the framework is general, in this paper we focus on the pair $(G,K) = (\mathrm{GL}_{2n}(\mathbb{C}), \mathrm{GL}_n(\mathbb{C}) \times \mathrm{GL}_n(\mathbb{C}))$. Then the generalized Steinberg map is a map from \emph{partial} permutations to the pairs of nilpotent orbits in $ \mathfrak{gl}_n(\mathbb{C}) $. It involves a generalization of the classical Robinson--Schensted correspondence to the case of partial permutations. The other map, the exotic moment map, establishes a combinatorial map from the set of partial permutations to that of signed Young diagrams, i.e., the set of nilpotent $K$-orbits in the Cartan space $(\mathrm{Lie}(G)/\mathrm{Lie}(K))^* $. We explain the geometric background of the theory and combinatorial algorithms which produce the above mentioned maps.

A generalization of Steinberg theory and an exotic moment map

Abstract

For a reductive group , Steinberg established a map from the Weyl group to the set of nilpotent -orbits by using moment maps on double flag varieties. In particular, in the case of the general linear group, it provides a geometric interpretation of the Robinson-Schensted correspondence between permutations and pairs of standard tableaux of the same shape. We extend Steinberg's approach to the case of a symmetric pair to obtain two different maps, namely a \emph{generalized Steinberg map} and an \emph{exotic moment map}. Although the framework is general, in this paper we focus on the pair . Then the generalized Steinberg map is a map from \emph{partial} permutations to the pairs of nilpotent orbits in . It involves a generalization of the classical Robinson--Schensted correspondence to the case of partial permutations. The other map, the exotic moment map, establishes a combinatorial map from the set of partial permutations to that of signed Young diagrams, i.e., the set of nilpotent -orbits in the Cartan space . We explain the geometric background of the theory and combinatorial algorithms which produce the above mentioned maps.

Paper Structure

This paper contains 35 sections, 31 theorems, 207 equations, 3 figures.

Key Result

Proposition 1.1

Assume that Then, the conormal variety $\mathcal{Y}$ is equidimensional and its irreducible components are in one-to-one correspondence with the $K$-orbits of $\mathfrak{X}$. More precisely, whenever $\mathbb{O}\subset\mathfrak{X}$ is a $K$-orbit, the closure of the conormal bundle $T^*_\mathbb{O}\mathfrak{X}$

Figures (3)

  • Figure 1: The correspondence $\tau\mapsto(T_1,T_2,\nu)$ for $\mathfrak{T}_3$ ($\mathrm{rank}\,\tau=3$); the maps $\Phi$, $\Xi_{\mathfrak{k}}$, and $\Xi_{\mathfrak{s}}$
  • Figure 2: The correspondence $\tau\mapsto(T_1,T_2,\nu)$ for $\mathfrak{T}_3$ ($\mathrm{rank}\,\tau=2$); the maps $\Phi$, $\Xi_{\mathfrak{k}}$, and $\Xi_{\mathfrak{s}}$
  • Figure 3: The correspondence $\tau\mapsto(T_1,T_2,\nu)$ for $\mathfrak{T}_3$ ($\mathrm{rank}\,\tau\leq 1$); the maps $\Phi$, $\Xi_{\mathfrak{k}}$, and $\Xi_{\mathfrak{s}}$

Theorems & Definitions (67)

  • Proposition 1.1
  • Remark 1.3
  • Theorem 1.4: see Theorem \ref{['T3']}
  • Theorem 1.5: Theorems \ref{['T4']} and \ref{['T5']}
  • Theorem 1.6
  • Theorem 1.7: Theorems \ref{['T2']} and \ref{['thm:3.9']}
  • Proposition 3.1
  • proof
  • Theorem 4.1: Steinberg2
  • Definition 5.1
  • ...and 57 more