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Schubert Cycle Expansion in Flag Varieties

Updated 21 October 2025
  • Schubert cycle expansion is the process of expressing (co)homology classes of Richardson varieties as linear combinations of Schubert classes, with coefficients derived from combinatorial and geometric data.
  • The expansion employs combinatorial models—such as (p,q)-clans in type A—to parameterize symmetric subgroup orbits and yield explicit, multiplicity-free structure constants.
  • This framework bridges geometry, combinatorics, and representation theory by offering subtraction-free formulas that simplify Schubert calculus and suggest extensions to other types like B and D.

Schubert cycle expansion refers to the representation of (co)homology classes of subvarieties of the flag variety—especially Richardson varieties—as linear combinations in the Schubert basis, with coefficients encoding fundamental geometric, combinatorial, or representation-theoretic information. In the context of Richardson varieties stable under spherical Levi subgroups, this expansion is governed by Brion’s theorem, combinatorial models parametrizing symmetric subgroup orbits, and explicit positivity results for the associated structure constants in several cases. The interplay of these elements yields manifestly positive, often multiplicity-free, combinatorial formulas for the expansion coefficients and establishes new connections between representation theory, geometry, and combinatorics.

1. Brion’s Theorem for Spherical Subgroup Orbits

The critical structural input is Brion’s theorem, which describes the expansion of the cohomology class of an orbit closure of a spherical subgroup HH on the flag variety G/BG/B in the Schubert basis. For a spherical subgroup HGH \leq G and an HH-orbit closure YG/BY \subset G/B: [Y]=wW(Y)2D(w)Sw[Y] = \sum_{w \in W(Y)} 2^{D(w)} \cdot S_w where:

  • W(Y)W(Y) is the set of Weyl group elements indexing paths in the weak order graph from YY to the dense orbit.
  • D(w)D(w) is the number of “double edges” (edges associated to noncompact imaginary roots of type II) encountered in (any) reduced expression for ww.

For a Richardson variety Xvu=XuXvX^u_v = X^u \cap X_v (intersection of a Schubert and an opposite Schubert variety), if XvuX^u_v is stable under a spherical Levi subgroup LL, it is the closure of an LL-orbit. Brion’s theorem then holds: [Xvu]=Sw0uSv=wW(Y)2D(w)Sw[X^u_v] = S_{w_0 u} \cdot S_v = \sum_{w \in W(Y)} 2^{D(w)} S_w where YY is the associated LL-orbit closure. In type A, all edges are simple, so 2D(w)=12^{D(w)} = 1, and the expansion is multiplicity-free.

2. Clans and the Combinatorial Model for Orbits

In type AA, the pair (G,L)=(GL(p+q,C),GL(p,C)×GL(q,C))(G, L) = (GL(p+q,\mathbb{C}), GL(p,\mathbb{C}) \times GL(q,\mathbb{C})) leads to an LL-orbit combinatorial model parametrized by (p,q)(p, q)-clans. A (p, q)-clan is a string on n=p+qn=p+q positions filled with “+”, “–”, or a natural number, with each number appearing exactly twice (up to relabeling), and the difference between “+” and “–” is pqp-q. The weak order on the closure relations among LL-orbit closures is governed by explicit operations on clans, corresponding to Weyl group reflections.

The action of a Weyl group element ww on a clan γ\gamma follows two primary rules: swapping entries at positions ii and i+1i+1 (unless these are opposite signs, in which case they are replaced with a new matching numeric symbol). Thus, a path in the weak order graph corresponds to a sequence of such operations, and structure constants can be read from the combinatorics of the action.

3. Explicit Schubert Structure Constants for Special Cases

For special permutations uu and vv (specifically, uu the inverse of a Grassmannian permutation with unique descent at pp, and vv inverse to one with unique descent at qq), the expansion coefficient cw0u,vwc_{w_0 u, v}^w is given by: cw0u,vw={1,wγ(u,v)=γ0 0,otherwisec_{w_0 u, v}^{w} = \begin{cases} 1, & w \cdot \gamma(u,v) = \gamma_0\ 0, & \text{otherwise} \end{cases} where γ(u,v)\gamma(u, v) is the clan associated to the pair (u,v)(u,v), γ0\gamma_0 is the dense LL-orbit clan, and ww is required to have length equal to the codimension of XvuX^u_v. This formula (Theorem 3.11) is positive and combinatorial: to determine the coefficient, one simply checks the action of ww on γ(u,v)\gamma(u, v) in the clan model.

In type AA, all edge multiplicities are one, so all coefficients in the expansion are 0 or 1.

4. Conjectures in Types B and D

For types BB and DD (i.e., G=SO(2n+1,C)G = SO(2n+1,\mathbb{C}) or SO(2n,C)SO(2n,\mathbb{C}) with LL a spherical Levi subgroup), the authors propose similar combinatorial expansions, conjecturing that:

  • For type BB, coefficients may take values $0$, $1$, or $2$—the value $2$ arises when a specific scenario occurs in the action of M(W)M(W) on the clan.
  • For type DD, coefficients remain $0$ or $1$.

The basic philosophy remains: construct a clan model for the LL-orbits, identify the closure corresponding to the Richardson variety, use Brion-type expansions (with possible double edges), and read off structure constants via combinatorics.

5. Positivity, Applications, and Implications

Key implications include:

  • All described structure constants in type AA (and conjecturally in types BB and DD) are positive (subtraction-free). This advances the program of providing positive formulas for Schubert structure constants, a central question in Schubert calculus.
  • The geometry of LL-orbit closures translates intersection theoretic computations into combinatorics on clans, linking geometric representation theory (via orbits and equivariant geometry) with explicit combinatorial algorithms.
  • This connection offers new perspectives on singularity properties (e.g., rational smoothness and pattern avoidance) and enables the study of Richardson varieties' local geometry.
  • Algorithmic computations for Schubert calculus benefit from this explicit expansion, with implications for computational representation theory frameworks, such as ATLAS.

6. Summary Table: Key Structural Ingredients

Aspect Type AA (GL) Type BB/DD (SO)
Orbit parametrization (p,q)(p,q)-clans symmetric clans (Matsuki–Oshima)
Expansion via Brion’s theorem [Y]=wSw[Y]=\sum_w S_w (multiplicity-free) [Y]=w2D(w)Sw[Y]=\sum_w 2^{D(w)} S_w
Expansion coefficient values $0, 1$ $0, 1$ (DD); $0, 1, 2$ (BB)
Coefficient computation wγ=γ0w \cdot \gamma = \gamma_0 condition as above, with possible $2$s
Application to positivity Unconditional Conjectural

7. Research Directions and Extensions

  • Extension of explicit combinatorial rules for structure constants beyond type AA remains an active direction, hinging on verifying conjectures for types BB and DD or constructing clan analogues.
  • The interface between local geometry (e.g., rational smoothness criteria) of Schubert varieties and the combinatorics of clans suggests new approaches for classification and singularity theory.
  • Since the expansion provides effective formulas computationally, implementing these rules in computational packages opens Schubert calculus to wider experimentation and large-scale data analysis.
  • The reduction to positivity using these expansions may have broader impact in neighboring domains, such as the theory of total positivity or the exploration of representation spaces of real forms.

The expansion of classes of Richardson varieties (stable under spherical Levi subgroups) in the Schubert basis, via Brion’s theorem and combinatorial models of orbits, provides not only subtraction-free structure constants for large classes but also structural bridges between geometry, combinatorics, and representation theory, offering new opportunities for theoretical development and computation in Schubert calculus (Wyser, 2012).

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