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In mathematics, the Grassmannian Gr(k, V) is a space which parametrizes all k-dimensional linear subspaces of the n-dimensional vector space V. For example, the Grassmannian Gr(1, V) is the space of lines through the origin in V, so it is the same as the projective space of one dimension lower than V.

When V is a real or complex vector space, Grassmannians are compact smooth manifolds.[1] In general they have the structure of a smooth algebraic variety, of dimension

The earliest work on a non-trivial Grassmannian is due to Julius Plücker, who studied the set of projective lines in projective 3-space, equivalent to Gr(2, R4) and parameterized them by what are now called Plücker coordinates. Hermann Grassmann later introduced the concept in general.

Notations vary between authors, with being equivalent to Gr(k, V), and some authors using or Gr(k, n) to denote the Grassmannian of k-dimensional subspaces of an unspecified n-dimensional vector space.


By giving a collection of subspaces of some vector space a topological structure, it is possible to talk about a continuous choice of subspace or open and closed collections of subspaces; by giving them the structure of a differential manifold one can talk about smooth choices of subspace.

A natural example comes from tangent bundles of smooth manifolds embedded in Euclidean space. Suppose we have a manifold M of dimension k embedded in Rn. At each point x in M, the tangent space to M can be considered as a subspace of the tangent space of Rn, which is just Rn. The map assigning to x its tangent space defines a map from M to Gr(k, n). (In order to do this, we have to translate the tangent space at each xM so that it passes through the origin rather than x, and hence defines a k-dimensional vector subspace. This idea is very similar to the Gauss map for surfaces in a 3-dimensional space.)

This idea can with some effort be extended to all vector bundles over a manifold M, so that every vector bundle generates a continuous map from M to a suitably generalised Grassmannian—although various embedding theorems must be proved to show this. We then find that the properties of our vector bundles are related to the properties of the corresponding maps viewed as continuous maps. In particular we find that vector bundles inducing homotopic maps to the Grassmannian are isomorphic. Here the definition of homotopic relies on a notion of continuity, and hence a topology.

Low dimensionsEdit

For k = 1, the Grassmannian Gr(1, n) is the space of lines through the origin in n-space, so it is the same as the projective space of n−1 dimensions.

For k = 2, the Grassmannian is the space of all 2-dimensional planes containing the origin. In Euclidean 3-space, a plane containing the origin is completely characterized by the one and only line through the origin that is perpendicular to that plane (and vice versa); hence the spaces Gr(2, 3), Gr(1, 3), and P2 (the projective plane) may all be identified with each other.

The simplest Grassmannian that is not a projective space is Gr(2, 4), which may be parameterized via Plücker coordinates.

The geometric definition of the Grassmannian as a setEdit

Let V be an  -dimensional vector space over a field K. The Grassmannian Gr(k, V) is the set of all k-dimensional linear subspaces of V. The Grassmannian is also denoted Gr(k, n) or  .

The Grassmannian as a differentiable manifoldEdit

To endow the Grassmannian   with the structure of a differentiable manifold, choose a basis for  . This is equivalent to identifying it with   with the standard basis, denoted  , viewed as column vectors. Then for any   dimensional subspace  , viewed as an element of  , we may choose a basis consisting of   linearly independent column vectors  . The homogeneous coordinates of the element   consist of the components of the   rectangular matrix   of maximal rank whose  th column vector is  . Since the choice of basis is arbitrary, two such maximal rank rectangular matrices   and   represent the same element   if and only if   for some element   of the general linear group of invertible   matrices with entries in  .

Now we define a coordinate atlas. For any   matrix  , we can apply elementary column operations to obtain its reduced column echelon form. If the first   rows of   are linearly independent, the result will have the form


The   matrix   determines  . In general, the first   rows need not be independent, but for any   whose rank is  , there exists an ordered set of integers   such that the submatrix   consisting of the  -th rows of   is nonsingular. We may apply column operations to reduce this submatrix to the identity, and the remaining entries uniquely correspond to  . Hence we have the following definition:

For each ordered set of integers  , let   be the set of   matrices   whose   submatrix   is nonsingular, where the  th row of   is the  th row of  . The coordinate function on   is then defined as the map   that sends   to the   rectangular matrix whose rows are the rows of the matrix   complementary to  . The choice of homogeneous coordinate matrix   representing the element   does not affect the values of the coordinate matrix   representing   on the coordinate neighbourhood  . Moreover, the coordinate matrices   may take arbitrary values, and they define a diffeomorphism from   onto the space of   dimensional  -valued matrices.

On the overlap


of any two such coordinate neighborhoods, the coordinate matrix values are related by the transition relation


where both   and   are invertible. Hence   gives an atlas of  .

The Grassmannian as a homogeneous spaceEdit

The quickest way of giving the Grassmannian a geometric structure is to express it as a homogeneous space. First, recall that the general linear group GL(V) acts transitively on the r-dimensional subspaces of V. Therefore, if H is the stabilizer of any of the subspaces under this action, we have

Gr(r, V) = GL(V)/H.

If the underlying field is R or C and GL(V) is considered as a Lie group, then this construction makes the Grassmannian into a smooth manifold. It also becomes possible to use other groups to make this construction. To do this, fix an inner product on V. Over R, one replaces GL(V) by the orthogonal group O(V), and by restricting to orthonormal frames, one gets the identity

Gr(r, n) = O(n)/(O(r) × O(nr)).

In particular, the dimension of the Grassmannian is r(nr).

Over C, one replaces GL(V) by the unitary group U(V). This shows that the Grassmannian is compact. These constructions also make the Grassmannian into a metric space: For a subspace W of V, let PW be the projection of V onto W. Then


where ||⋅|| denotes the operator norm, is a metric on Gr(r, V). The exact inner product used does not matter, because a different inner product will give an equivalent norm on V, and so give an equivalent metric.

If the ground field k is arbitrary and GL(V) is considered as an algebraic group, then this construction shows that the Grassmannian is a non-singular algebraic variety. It follows from the existence of the Plücker embedding that the Grassmannian is complete as an algebraic variety. In particular, H is a parabolic subgroup of GL(V).

The Grassmannian as a schemeEdit

In the realm of algebraic geometry, the Grassmannian can be constructed as a scheme by expressing it as a representable functor.[2]

Representable functorEdit

Let   be a quasi-coherent sheaf on a scheme S. Fix a positive integer r. Then to each S-scheme T, the Grassmannian functor associates the set of quotient modules of


locally free of rank r on T. We denote this set by  .

This functor is representable by a separated S-scheme  . The latter is projective if   is finitely generated. When S is the spectrum of a field k, then the sheaf   is given by a vector space V and we recover the usual Grassmannian variety of the dual space of V, namely: Gr(r, V).

By construction, the Grassmannian scheme is compatible with base changes: for any S-scheme S′, we have a canonical isomorphism


In particular, for any point s of S, the canonical morphism {s} = Spec(k(s)) → S, induces an isomorphism from the fiber   to the usual Grassmannian   over the residue field k(s).

Universal familyEdit

Since the Grassmannian scheme represents a functor, it comes with a universal object,  , which is an object of


and therefore a quotient module   of  , locally free of rank r over  . The quotient homomorphism induces a closed immersion from the projective bundle  :


For any morphism of S-schemes:


this closed immersion induces a closed immersion


Conversely, any such closed immersion comes from a surjective homomorphism of OT-modules from   to a locally free module of rank r.[3] Therefore, the elements of   are exactly the projective subbundles of rank r in


Under this identification, when T = S is the spectrum of a field k and   is given by a vector space V, the set of rational points   correspond to the projective linear subspaces of dimension r − 1 in P(V), and the image of   in


is the set


The Plücker embeddingEdit

The Plücker embedding is a natural embedding of the Grassmannian   into the projectivization of the exterior algebra  :


Suppose that W is a k-dimensional subspace of the   dimensional vector space V. To define  , choose a basis {w1, ..., wk}, of W, and let   be the wedge product of these basis elements:


A different basis for W will give a different wedge product, but the two products will differ only by a non-zero scalar (the determinant of the change of basis matrix). Since the right-hand side takes values in a projective space,   is well-defined. To see that   is an embedding, notice that it is possible to recover   from   as the span of the set of all vectors   such that  .

Plücker coordinates and the Plücker relationsEdit

The Plücker embedding of the Grassmannian satisfies some very simple quadratic relations called the Plücker relations. These show that the Grassmannian embeds as an algebraic subvariety of P(∧kV) and give another method of constructing the Grassmannian. To state the Plücker relations, fix a basis {e1, ..., en} of V, and let W be a k-dimensional subspace of V with basis {w1, ..., wk}. Let (wi1, ..., win) be the coordinates of wi with respect to the basis {e1, ..., en} of V, let

and let {W1, ..., Wn} be the columns of  . For any ordered sequence   of   positive integers, let   be the determinant of the   matrix with columns  . The set   is called the Plücker coordinates of the element   of the Grassmannian (with respect to the basis {e1, ..., en} of V). They are the linear coordinates of the image   of   under the Plücker map, relative to the basis of the exterior power  induced by the basis {e1, ..., en} of V.

For any two ordered sequences   and   of   and   positive integers, resp., the following homogeneous equations are valid and determine the image of W under the Plücker embedding:


where   denotes the sequence   with the term   omitted.

When dim(V) = 4, and k = 2, the simplest Grassmannian which is not a projective space, the above reduces to a single equation. Denoting the coordinates of P(∧kV) by W12, W13, W14, W23, W24, W34, the image of Gr(2, V) under the Plücker map is defined by the single equation

W12W34W13W24 + W23W14 = 0.

In general, however, many more equations are needed to define the Plücker embedding of a Grassmannian in projective space.[4]

The Grassmannian as a real affine algebraic varietyEdit

Let Gr(r, Rn) denote the Grassmannian of r-dimensional subspaces of Rn. Let M(n, R) denote the space of real n × n matrices. Consider the set of matrices A(r, n) ⊂ M(n, R) defined by XA(r, n) if and only if the three conditions are satisfied:

  • X is a projection operator: X2 = X.
  • X is symmetric: Xt = X.
  • X has trace r: tr(X) = r.

A(r, n) and Gr(r, Rn) are homeomorphic, with a correspondence established by sending XA(r, n) to the column space of X.


Every r-dimensional subspace W of V determines an (nr)-dimensional quotient space V/W of V. This gives the natural short exact sequence:

0 → WVV/W → 0.

Taking the dual to each of these three spaces and linear transformations yields an inclusion of (V/W) in V with quotient W:

0 → (V/W)VW → 0.

Using the natural isomorphism of a finite-dimensional vector space with its double dual shows that taking the dual again recovers the original short exact sequence. Consequently there is a one-to-one correspondence between r-dimensional subspaces of V and (nr)-dimensional subspaces of V. In terms of the Grassmannian, this is a canonical isomorphism

Gr(r, V) ≅ Gr(nr, V).

Choosing an isomorphism of V with V therefore determines a (non-canonical) isomorphism of Gr(r, V) and Gr(nr, V). An isomorphism of V with V is equivalent to a choice of an inner product, and with respect to the chosen inner product, this isomorphism of Grassmannians sends an r-dimensional subspace into its (nr)-dimensional orthogonal complement.

Schubert cellsEdit

The detailed study of the Grassmannians uses a decomposition into subsets called Schubert cells, which were first applied in enumerative geometry. The Schubert cells for Gr(r, n) are defined in terms of an auxiliary flag: take subspaces V1, V2, ..., Vr, with ViVi + 1. Then we consider the corresponding subset of Gr(r, n), consisting of the W having intersection with Vi of dimension at least i, for i = 1, ..., r. The manipulation of Schubert cells is Schubert calculus.

Here is an example of the technique. Consider the problem of determining the Euler characteristic of the Grassmannian of r-dimensional subspaces of Rn. Fix a 1-dimensional subspace RRn and consider the partition of Gr(r, n) into those r-dimensional subspaces of Rn that contain R and those that do not. The former is Gr(r − 1, n − 1) and the latter is a r-dimensional vector bundle over Gr(r, n − 1). This gives recursive formulas:


If one solves this recurrence relation, one gets the formula: χr, n = 0 if and only if n is even and r is odd. Otherwise:


Cohomology ring of the complex GrassmannianEdit

Every point in the complex Grassmannian manifold Gr(r, n) defines an r-plane in n-space. Fibering these planes over the Grassmannian one arrives at the vector bundle E which generalizes the tautological bundle of a projective space. Similarly the (nr)-dimensional orthogonal complements of these planes yield an orthogonal vector bundle F. The integral cohomology of the Grassmannians is generated, as a ring, by the Chern classes of E. In particular, all of the integral cohomology is at even degree as in the case of a projective space.

These generators are subject to a set of relations, which defines the ring. The defining relations are easy to express for a larger set of generators, which consists of the Chern classes of E and F. Then the relations merely state that the direct sum of the bundles E and F is trivial. Functoriality of the total Chern classes allows one to write this relation as


The quantum cohomology ring was calculated by Edward Witten in The Verlinde Algebra And The Cohomology Of The Grassmannian. The generators are identical to those of the classical cohomology ring, but the top relation is changed to


reflecting the existence in the corresponding quantum field theory of an instanton with 2n fermionic zero-modes which violates the degree of the cohomology corresponding to a state by 2n units.

Associated measureEdit

When V is n-dimensional Euclidean space, one may define a uniform measure on Gr(r, n) in the following way. Let θn be the unit Haar measure on the orthogonal group O(n) and fix V in Gr(r, n). Then for a set AGr(r, n), define


This measure is invariant under actions from the group O(n), that is, γr, n(gA) = γr, n(A) for all g in O(n). Since θn(O(n)) = 1, we have γr, n(Gr(r, n)) = 1. Moreover, γr, n is a Radon measure with respect to the metric space topology and is uniform in the sense that every ball of the same radius (with respect to this metric) is of the same measure.

Oriented GrassmannianEdit

This is the manifold consisting of all oriented r-dimensional subspaces of Rn. It is a double cover of Gr(r, n) and is denoted by:


As a homogeneous space it can be expressed as:



Grassmann manifolds have found application in computer vision tasks of video-based face recognition and shape recognition.[5] They are also used in the data-visualization technique known as the grand tour.

Grassmannians allow the scattering amplitudes of subatomic particles to be calculated via a positive Grassmannian construct called the amplituhedron.[6]

See alsoEdit


  1. ^ Milnor & Stasheff (1974), pp. 57–59.
  2. ^ Grothendieck, Alexander (1971). Éléments de géométrie algébrique. 1 (2nd ed.). Berlin, New York: Springer-Verlag. ISBN 978-3-540-05113-8., Chapter I.9
  3. ^ EGA, II.3.6.3.
  4. ^ Griffiths, Phillip; Harris, Joseph (1994), Principles of algebraic geometry, Wiley Classics Library (2nd ed.), New York: John Wiley & Sons, p. 211, ISBN 0-471-05059-8, MR 1288523, Zbl 0836.14001
  5. ^ Pavan Turaga, Ashok Veeraraghavan, Rama Chellappa: Statistical analysis on Stiefel and Grassmann manifolds with applications in computer vision, CVPR 23–28 June 2008, IEEE Conference on Computer Vision and Pattern Recognition, 2008, ISBN 978-1-4244-2242-5, pp. 1–8 (abstract, full text)
  6. ^ Arkani-Hamed, Nima; Trnka, Jaroslav (2013). "The Amplituhedron". Journal of High Energy Physics. 2014 (10). arXiv:1312.2007. Bibcode:2014JHEP...10..030A. doi:10.1007/JHEP10(2014)030.
  7. ^ Morel, Fabien; Voevodsky, Vladimir (1999). "A^1-homotopy theory of schemes" (PDF). Publications Mathématiques de l'IHÉS. 90 (90): 45–143. doi:10.1007/BF02698831. ISSN 1618-1913. MR 1813224. Retrieved 2008-09-05., see section 4.3., pp. 137–140