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Plücker Ray Maps: Grassmannian & Isotropic Geometry

Updated 19 December 2025
  • Plücker ray maps are canonical projective embeddings that associate each N-plane with its decomposable exterior wedge product, defining a unique projective ray.
  • They enable a deep connection between Plücker coordinates and Cartan (spinor) maps by linking determinants with Pfaffian line bundles through bilinear identities.
  • This framework underpins applications in integrable systems and representation theory, offering explicit coordinate relations and a bridge between algebraic and geometric invariants.

The Plücker map, often referred to in projective-geometric contexts as a "ray map," provides a canonical embedding of a Grassmannian into a projective space by associating to each NN-plane its exterior wedge product—a decomposable NN-vector, thus identifying each point with a unique projective ray. In the context of the vector space W=VVW=V\oplus V^*, where VV is an NN-dimensional complex vector space, this embedding plays a foundational role in relating the geometry of general and isotropic Grassmannians. Its structure also facilitates profound links with the theory of Cartan (spinor) maps, Pfaffian line bundles, and determinant identities of Cauchy-Binet type, particularly on the locus of maximal isotropic subspaces. The key results and constructions in this domain are summarized and rigorously developed in (Balogh et al., 2020).

1. Plücker Embedding and Ray Assignment

Let VV be a complex vector space of dimension NN and VV^* its dual. Consider W=VVW=V\oplus V^*, and the Grassmannian GrN(W)Gr_N(W) of NN-dimensional subspaces wWw\subset W. For any basis w={w1,,wN}w=\{w_1,\dots,w_N\} of such a subspace, the exterior product w1wNNWw_1\wedge\cdots\wedge w_N\in\wedge^N W defines a projective equivalence class (a "ray") in P(NW)\mathbb P(\wedge^N W). The classical Plücker map

$\mathrm{Pl}\;:=\;\Blv:\;Gr_N(W)\;\longrightarrow\;\mathbb P(\wedge^N W),\quad \Blv(\mathrm{span}\{w_1,\dots,w_N\})=[w_1\wedge\cdots\wedge w_N]$

is thus viewed as the canonical "Plücker ray map". Each point of the Grassmannian is associated with a unique line (projective ray) in NW\wedge^N W. The map acts compatibly with projective lines: a one-parameter family w(t)w(t) in the Grassmannian traces a projective line in P(NW)\mathbb P(\wedge^N W) under $\Blv$.

The Plücker coordinates are indexed by partitions λ\lambda whose Young diagrams fit within an N×NN\times N square. In a combined basis {e1,,eN,f1,,fN}\{e_1,\dots,e_N,f_1,\dots,f_N\} for WW, the decomposable NN-vector can be expanded as

$\Blv(w)=\sum_{\lambda\subseteq(N^N)} T_\lambda(w) |\lambda\rangle$

where Tλ(w)=detWλ(w)T_\lambda(w)=\det W_\lambda(w) for each N×NN\times N minor Wλ(w)W_\lambda(w) determined by multi-index λ\lambda.

2. Isotropic Grassmannians and the Cartan (Spinor) Map

On W=VVW=V\oplus V^*, introduce the canonical nondegenerate pairing Q((X,p),(Y,q))=q(X)+p(Y)Q((X,p),(Y,q))=q(X)+p(Y) for X,YVX,Y\in V, p,qVp,q\in V^*. The isotropic Grassmannian $\Gr^0(W,Q)$ consists of NN-planes w0w^0 such that Q(wi,wj)=0Q(w_i,w_j)=0 for all i,ji,j.

Cartan’s construction realizes V\wedge V as an irreducible Clifford (spinor) module under the action of

Γv=v+ivEnd(V)\Gamma_v = v\wedge + i_v \in \operatorname{End}(\wedge V)

where vWv\in W acts by exterior and interior multiplication. For a maximal isotropic NN-plane w0=span(w1,,wN)w^0=\mathrm{span}(w_1,\dots,w_N), the operator product Γw1Γw2ΓwN\Gamma_{w_1}\Gamma_{w_2}\cdots\Gamma_{w_N} yields a pure spinor in V\wedge V. The Cartan embedding is then

$\Cay:\;\Gr^0(W,Q) \rightarrow \mathbb P(\wedge V),\quad \Cay(w^0)= [\Gamma_{w_1}\cdots\Gamma_{w_N}]$

The homogeneous coordinates ka(w0)k_a(w^0)—Cartan coordinates—are labeled by strict partitions a=(a1>>ar)a=(a_1>\cdots>a_r) and are given by

ka(w0)=(1)Pf(A(a)(w0))k_a(w^0) = (-1)^{\cdots}\operatorname{Pf}(A^{(a)}(w^0))

where A(w0)A(w^0) is the skew-symmetric N×NN\times N affine coordinate matrix, and A(a)(w0)A^{(a)}(w^0) is the principal r×rr\times r submatrix.

3. Coordinate Description: Plücker and Cartan Systems

The Plücker coordinates Tλ(w)T_\lambda(w) arise as determinants of N×NN\times N minors extracted from the 2N×N2N\times N coordinate matrix W(w)W(w) of the NN-plane wWw\subset W. For isotropic NN-planes, affine coordinates A(w0)A(w^0) parameterize the "big cell" in the Grassmannian, and the Cartan coordinates are determined as Pfaffians of principal submatrices.

Object Coordinates Explicit Construction
General NN-plane ww Plücker Tλ(w)T_\lambda(w) detWλ(w)\det W_\lambda(w)
Isotropic NN-plane w0w^0 Cartan ka(w0)k_a(w^0) (1)PfA(a)(w0)(-1)^{\cdots} \operatorname{Pf}A^{(a)}(w^0)

This coordinate system enables explicit computations and forms the basis for the bilinear relations between these two embeddings on the isotropic locus.

4. Bilinear Identities: Cauchy–Binet–Pfaffian Relation

A fundamental connection arises between the Plücker and Cartan embeddings through a quadratic map BN:V×VNWB_N:\wedge V\times\wedge V\rightarrow\wedge^N W induced by the spin–pairing. Explicitly, for the isotropic locus, one has

$B_N(\Cay(w^0),\Cay(w^0)) = \Blv(w^0)\quad\text{in}\;\mathbb P(\wedge^N W)$

in particular, the image of the Cartan map under this quadratic spinor pairing is precisely the Plücker image.

In coordinates, this gives a Pfaffian analogue of the Cauchy–Binet formula. Let A(w0)A(w^0) be the affine coordinate matrix, and I,J{1,,N}I, J\subset\{1,\dots, N\}, I=J=r|I|=|J|=r, then for A(IJ)A(I|J) the r×rr\times r submatrix,

detA(IJ)=2r(1)r(r1)2K,Leven KL=IJ KL=IJ(1)rd+v(I,J,K,L)PfA(KK)PfA(LL)\det A(I|J) = 2^r\, (-1)^{\frac{r(r-1)}2} \sum_{ \substack{ K,L\;\mathrm{even}\ K\cup L=I\cup J\ K\cap L=I\cap J } } (-1)^{r d+v(I,J,K,L)}\, \operatorname{Pf}A(K|K)\, \operatorname{Pf}A(L|L)

where the exponents dd and v(I,J,K,L)v(I,J,K,L) are combinatorial. Thus, each Plücker coordinate is bilinear in the Cartan coordinates, precisely reflecting the factorization through the Segre embedding.

5. Geometric Interplay: Line Bundles and Embedding Factorization

The Plücker embedding realizes GrN(VV)Gr_N(V\oplus V^*) as the variety of decomposable NN-vectors in P(N(VV))\mathbb P(\wedge^N(V\oplus V^*)), with each point corresponding to a "ray." Projective lines in the Grassmannian are mapped to projective lines in the image. On $\Gr^0(V\oplus V^*,Q)$, the Cartan map produces a subvariety of pure spinors in P(V)\mathbb P(\wedge V), with homogeneous Cartan coordinates realizing holomorphic sections of the dual Pfaffian line bundle $\mathrm{Pf}^*\to\Gr^0$.

A central identity identifies the restriction of the determinantal line bundle DetGrN\mathrm{Det}^*\to Gr_N to $\Gr^0$ in terms of the square of the Pfaffian line bundle, and expresses the Plücker embedding as the composite of the Segre embedding

P(V)×P(V)P(N(VV))\mathbb P(\wedge V)\times\mathbb P(\wedge V)\to\mathbb P(\wedge^N(V\oplus V^*))

with the Cartan map diagonally. This shows that on isotropic NN-planes, the determinant-type Plücker coordinates factor through the quadratic pairing of spinor-type (Pfaffian) coordinates.

6. Context and Implications in Representation and Integrable Systems

The framework is motivated by, and directly applies to, the study of τ\tau-functions of the KP and BKP integrable hierarchies, which are interpreted as sections of determinantal and Pfaffian line bundles over infinite-dimensional Grassmannians. In finite-dimensional settings, these maps make explicit the interplay of exterior algebra, Clifford modules, and projective geometry.

This approach establishes important links between classical invariants in linear algebra (determinants, Pfaffians), projective algebraic geometry, and the representation theory of symmetric spaces, with far-reaching consequences for the study of integrable systems, representation theory of Lie algebras, and the geometry of moduli spaces (Balogh et al., 2020).

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