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Matsuki Orbits: Duality in CR-Geometry

Updated 24 September 2025
  • Matsuki orbits are intersections of real and complex group orbits in flag varieties, defined by their compact CR-structure and duality between real and symmetric subgroups.
  • They are analyzed using orbit decomposition theorems, fiber bundle models, and finiteness criteria, which are crucial for representation theory and analytic extensions.
  • Their applications span the study of CR-manifolds, cycle spaces, and geometric embeddings in semisimple Lie groups and symmetric spaces.

A Matsuki orbit is the intersection of a real group orbit and a complex group orbit in a flag variety or, more generally, in a complex homogeneous space, often endowed with a CR-structure induced by its embedding in the ambient complex manifold. Matsuki orbits and their geometric, analytic, and representation-theoretic properties underpin central dualities and orbit stratifications in the theory of semisimple Lie groups, symmetric spaces, and complex geometry. Techniques for analyzing Matsuki orbits include various orbit decomposition theorems, dualities, and the use of fiber bundle structures, as well as connections to the theory of CR-manifolds and cycle spaces.

1. Orbit Structure and Matsuki Duality

Matsuki duality refers to the phenomenon whereby orbits of a real form G0G_0 and a symmetric subgroup KK of a complex semisimple Lie group GG on a complex flag manifold M=G/QM=G/Q are in bijection, with the intersection of corresponding orbits forming compact orbits (sometimes called "Matsuki orbits"). Specifically, for each pMp\in M,

M+(p)=G0p,M(p)=Kp,M0(p)=K0p,M_+(p) = G_0 \cdot p, \quad M_-(p) = K \cdot p, \quad M_0(p) = K_0 \cdot p,

and there is a unique KK-orbit M(p)M_-(p_-) dual to each G0G_0-orbit M+(p+)M_+(p_+) such that their intersection is the compact K0K_0-orbit M0(p0)M_0(p_0): M+(p+)M(p)=M0(p0).M_+(p_+) \cap M_-(p_-) = M_0(p_0). This setup induces a finite and mutually dual collection of real and complex orbits, with the Matsuki orbits serving as the unique compact intersections (Marini et al., 2016). The duality is constructed via suitable choices of Borel and Cartan subalgebras and is a powerful tool for understanding representation-theoretic phenomena and geometric structures on flag varieties.

2. Open Orbit Criterion, Spherical Subgroups, and Finiteness

Theorem 1.1 in (Krötz et al., 2013) establishes that a closed connected subgroup HH of a connected real semisimple group GG admits an open orbit on the flag manifold G/PG/P (PP a minimal parabolic subgroup) if and only if HH has finitely many orbits on G/PG/P. The open HH-orbit condition admits an algebraic reformulation: g=h+Ad(x)p\mathfrak{g} = \mathfrak{h} + \mathrm{Ad}(x)\mathfrak{p} for some xGx\in G, with g,h,p\mathfrak{g}, \mathfrak{h}, \mathfrak{p} denoting the Lie algebras of G,H,PG, H, P respectively. Subgroups satisfying this condition are called (real) spherical subgroups. The converse is elementary, but the key content is that existence of an open orbit forces the finiteness: orbit stratifications for (real) spherical subgroups on real flag manifolds are always finite. Reduction to the real rank one case, and analysis of both reductive and non-reductive subgroups, are the technical heart of the proof. In the reductive case, the argument invokes the existence of a symmetric subgroup HH' such that the HH- and HH'-orbit structures on G/PG/P coincide.

3. Geometric Models: Fiber Bundles and CR-Structures

Matsuki orbits often admit a geometric model as compact homogeneous CR-submanifolds of flag varieties or Grassmannians. A prototypical construction appears in the context of complex Grassmannians: M,m,r=O,mO,m,rM_{\ell, m, r} = O_{\ell, m} \cap O_{\ell, m, r} where O,mO_{\ell, m} is a KK-orbit of kk-planes WW in V=E+EV = E_+ \oplus E_- with dim(WE+)=, dim(WE)=m\dim(W \cap E_+) = \ell,\ \dim(W \cap E_-) = m and O,m,rO_{\ell, m, r} is a G0G_0-orbit determined by an additional parameter r=kmr = k - \ell - m and a signature. O,mO_{\ell, m} is a smooth holomorphic fiber bundle over

B=Gr(E+)×Grm(E),B = \mathrm{Gr}_\ell(E_+) \times \mathrm{Gr}_m(E_-),

with typical fiber an open KK-orbit in a complementary Grassmannian. The Matsuki orbit M,m,rM_{\ell, m, r} forms a compact CR-submanifold, with CR-bundle

HM,m,r=T(1,0)O,mM,m,rTCM,m,r.H_{M_{\ell,m,r}} = T^{(1,0)}O_{\ell,m}|_{M_{\ell,m,r}} \cap T_\mathbb{C} M_{\ell,m,r}.

Explicitly, M,m,rM_{\ell,m,r} is the intersection of two maximal-dimensional orbits and inherits its CR-structure from the ambient geometry (Ullah, 21 Sep 2025, Marini et al., 2016).

4. Envelopes of Holomorphy and Holomorphic Extension

Given a compact homogeneous CR-submanifold M,m,rM_{\ell,m,r} as above, Rossi's theory applies: the envelope of holomorphy M^,m,r\hat{M}_{\ell, m, r} is the largest domain to which every CR-function on M,m,rM_{\ell, m, r} extends holomorphically. The key result in (Ullah, 21 Sep 2025) shows

M^,m,rO,m\hat{M}_{\ell, m, r} \cong O_{\ell, m}

biholomorphically. The proof uses the holomorphic fiber bundle structure π:O,mB\pi: O_{\ell, m} \to B and the compactness of the isotropic Grassmannian fibers within Matsuki orbits. Since any holomorphic (or CR) function on the total space must be locally constant along the compact fibers (by Liouville's theorem), every CR-function descends to a holomorphic function on the base. It follows that

OCR(M,m,r)=πO(B)\mathscr{O}_{CR}(M_{\ell, m, r}) = \pi^*\mathscr{O}(B)

and thus every CR-function on M,m,rM_{\ell, m, r} extends (uniquely) to a holomorphic function on the full KK-orbit O,mO_{\ell, m}.

5. Implications for Representation Theory and Complex Geometry

Finiteness of orbit stratifications and Matsuki duality are pivotal in harmonic analysis and representation theory for real semisimple Lie groups. Decomposing flag manifolds into finitely many orbits supports the analysis of branching, restriction problems, and multiplicity-freeness in representation theory (Krötz et al., 2013). The explicit geometric fiber bundle structures of Matsuki orbits support the construction of canonical complex embeddings of compact CR manifolds, enabling comparison of Dolbeault and CR cohomologies (Marini et al., 2016). These structures also have consequences for the paper of cycle spaces, analytic extensions of matrix coefficients, and for the geometric analysis of cycle spaces and crowns in the context of bounded symmetric domains and their compactifications (Olafsson et al., 2019).

6. Classical and Modern Examples

Typical examples include orbits in complex Grassmannians:

  • For V=C8V = \mathbb{C}^8 with signature(2,6)\mathrm{signature}(2,6), the Matsuki orbit M1,1,1Gr3(C8)M_{1,1,1} \subset \mathrm{Gr}_3(\mathbb{C}^8) is the intersection of the KK-orbit of 3-planes with one-dimensional intersection with E+E_+ and EE_-, and the G0G_0-orbit specified by an additional signature parameter. The envelope of holomorphy recovers the full KK-orbit O1,1O_{1,1}.

Broader classes of examples arise in settings such as ind-varieties of generalized flags (Fresse et al., 2017), affine Grassmannians (Chen et al., 2018), and cycle spaces (Olafsson et al., 2019), indicating the wide applicability of the orbit-theoretic and CR-geometric structures associated with Matsuki orbits. Special cases can be computed explicitly, revealing the deep links to combinatorial parametrizations and boundary phenomena in complex algebraic geometry.

7. Canonical Formulas and Structural Summary

Central formulas and constructions for Matsuki orbits in this context include:

Concept Structural Formula / Notion Context
Matsuki orbit definition M,m,r=O,mO,m,rM_{\ell,m,r}= O_{\ell,m} \cap O_{\ell,m,r} Intersection in Grassmannians
KK-orbit structure O,m={W:dim(WE+)=,dim(WE)=m}O_{\ell,m} = \{ W: \dim(W\cap E_+) = \ell, \dim(W\cap E_-) = m\} Holomorphic fiber bundle over BB
CR-bundle HM,m,r=T(1,0)O,mM,m,rTCM,m,rH_{M_{\ell,m,r}} = T^{(1,0)}O_{\ell,m}|_{M_{\ell,m,r}} \cap T_\mathbb{C} M_{\ell, m, r} Inherited CR-structure
Envelope of holomorphy M^,m,rO,m\hat{M}_{\ell, m, r} \cong O_{\ell, m} Maximal complex extension
CR-function algebra OCR(M,m,r)=πO(B)\mathscr{O}_{CR}(M_{\ell, m, r}) = \pi^*\mathscr{O}(B) Descent via fiber bundle

The geometric, analytic, and algebraic structure of Matsuki orbits thus provides a robust setting for linking real Lie group actions, complex geometry, and analytic extension problems. The invariance under group actions, the fiber bundle decompositions, and the rigidity of holomorphic extension phenomena all combine to make Matsuki orbits central objects in the intersection of representation theory, CR-geometry, and complex homogeneous dynamics (Krötz et al., 2013, Marini et al., 2016, Ullah, 21 Sep 2025).

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