Plücker embedding

Denoting by ${\displaystyle V=K^{n}}$ the ${\displaystyle n}$-dimensional vector space over the field ${\displaystyle K}$, and by ${\displaystyle \mathbf {Gr} (k,V)}$ the Grassmannian of ${\displaystyle k}$-dimensional subspaces of ${\displaystyle V}$, the Plücker embedding is the map ι defined by

${\displaystyle {\begin{aligned}\iota \colon \mathbf {Gr} (k,V)&{}\rightarrow \mathbf {P} (\Lambda ^{k}V),\\\iota \colon {\mathcal {W}}:=\operatorname {span} (w_{1},\ldots ,w_{k})&{}\mapsto [w_{1}\wedge \cdots \wedge w_{k}],\end{aligned}}}$

where ${\displaystyle (w_{1},\dots ,w_{k})}$ is a basis for the element ${\displaystyle {\mathcal {W}}\in \mathbf {Gr} (k,V)}$ and ${\displaystyle [w_{1}\wedge \cdots \wedge w_{k}]}$ is the projective equivalence class of the element ${\displaystyle w_{1}\wedge \cdots \wedge w_{k}\in \Lambda ^{k}V}$ of the ${\displaystyle k}$th exterior power of ${\displaystyle V}$.

This is an embedding of the Grassmannian into the projectivization ${\displaystyle \mathbf {P} (\Lambda ^{k}V)}$. The image can be completely characterized as the intersection of a number of quadrics, the Plücker quadrics (see below), which are expressed by homogeneous quadratic relations on the Plücker coordinates (see below) that derive from linear algebra.

The bracket ring appears as the ring of polynomial functions on ${\displaystyle \Lambda ^{k}V}$.[1]

The image under the Plücker embedding satisfies a simple set of homogeneous quadratic relations, usually called the Plücker relations, or Grassmann–Plücker relations, defining the intersection of a number of quadrics in ${\displaystyle \mathbf {P} (\Lambda ^{k}V)}$. This shows that the Grassmannian embeds as an algebraic subvariety of ${\displaystyle \mathbf {P} (\Lambda ^{k}V)}$ and gives another method of constructing the Grassmannian. To state the Grassmann–Plücker relations, let ${\displaystyle {\mathcal {W}}\in \mathbf {Gr} (k,V)}$ be the ${\displaystyle k}$-dimensional subspace spanned by the basis represented by column vectors ${\displaystyle W_{1},\dots ,W_{k}}$. Let ${\displaystyle W}$ be the ${\displaystyle n\times k}$ matrix of homogeneous coordinates, whose columns are ${\displaystyle W_{1},\dots ,W_{k}}$. Then the equivalence class ${\displaystyle [W]}$ of all such homogeneous coordinates matrices ${\displaystyle Wg\sim W}$ related to each other by right multiplication by an invertible ${\displaystyle k\times k}$ matrix ${\displaystyle g\in \mathbf {GL} (k,K)}$ may be identified with the element ${\displaystyle {\mathcal {W}}}$. For any ordered sequence ${\displaystyle 1\leq i_{1}<\cdots <i_{k}\leq n}$ of ${\displaystyle k}$ integers, let ${\displaystyle W_{i_{1},\dots ,i_{k}}}$ be the determinant of the ${\displaystyle k\times k}$ matrix whose rows are the rows ${\displaystyle (i_{1},\dots i_{k})}$ of ${\displaystyle W}$. Then, up to projectivization, ${\displaystyle \{W_{i_{1},\dots ,i_{k}}\}}$ are the Plücker coordinates of the element ${\displaystyle {\mathcal {W}}\sim [W]\in \mathbf {Gr} (k,V)}$ whose homogeneous coordinates are ${\displaystyle W}$. They are the linear coordinates of the image ${\displaystyle \iota ({\mathcal {W}})}$ of ${\displaystyle {\mathcal {W}}\in \mathbf {Gr} (k,V)}$ under the Plücker map, relative to the standard basis in the exterior space ${\displaystyle \Lambda ^{k}V}$. Changing the basis defining the homogeneous coordinate matrix ${\displaystyle M}$ just changes the Plücker coordinates by a nonzero scaling factor equal to the determinant of the change of basis matrix ${\displaystyle g}$, and hence just the representative of the projective equivalence class in ${\displaystyle \Lambda ^{k}V}$.

For any two ordered sequences:

${\displaystyle i_{1}<i_{2}<\cdots <i_{k-1},\quad j_{1}<j_{2}<\cdots <j_{k+1}}$

of positive integers ${\displaystyle 1\leq i_{l},j_{m}\leq n}$, the following homogeneous equations are valid, and determine the image of ${\displaystyle {\mathcal {W}}}$ under the Plücker map:[2]

${\displaystyle \sum _{l=1}^{k+1}(-1)^{l}W_{i_{1},\dots ,i_{k-1},j_{l}}W_{j_{1},\dots ,{\hat {j}}_{l},\dots j_{k+1}}=0,}$

(1)

where ${\displaystyle j_{1},\dots ,{\hat {j}}_{l}\dots j_{k+1}}$ denotes the sequence ${\displaystyle j_{1},\dots ,\dots j_{k+1}}$ with the term ${\displaystyle j_{l}}$ omitted. These are generally referred to as the Plücker relations.

When dim(V) = 4 and k = 2, we get ${\displaystyle \mathbf {Gr} (2,V)}$, the simplest Grassmannian which is not a projective space, and the above reduces to a single equation. Denoting the coordinates of ${\displaystyle \Lambda ^{2}V}$ by

${\displaystyle W_{ij}=-W_{ji},\quad 1\leq i,j,\leq 4,}$

the image of ${\displaystyle \mathbf {Gr} (2,V)}$ under the Plücker map is defined by the single equation

${\displaystyle W_{12}W_{34}-W_{13}W_{24}+W_{14}W_{23}=0.}$

In general, many more equations are needed to define the image of the Plücker embedding, as in (1), but these are not, in general, algebraically independent. The maximal number of algebraically independent relations (on Zariski open sets) is given by the difference of dimension between ${\displaystyle \mathbf {P} (\Lambda ^{k}V)}$ and ${\displaystyle \mathbf {Gr} (k,V)}$, which is ${\displaystyle n!/(k!(n-k)!)-n(n-k)-1.}$

• Miller, Ezra; Sturmfels, Bernd (2005). Combinatorial commutative algebra. Graduate Texts in Mathematics. Vol. 227. New York, NY: Springer-Verlag. ISBN 0-387-23707-0. Zbl 1090.13001.