*For an element z=0 of ⋀p(E) to be pure, it is necessary and sufficient that, for all u∗∈⋀p−1(E∗),
(u∗⊥z)∧z=0.
The case p=0 is trivial and we assume p≥1. If z=x1∧⋯∧xp, formula (68) (no. 9) with n=p−1 shows that u∗⊥z is a linear combination of the xi (1≤i≤p), whence (81). If on the other hand the subspace Mz associated with z is of dimension >p, consider a basis (ej)1≤j≤n of this subspace with n>p. It follows from no. 11, Proposition 13 that each of the ej is of the form u∗⊥z for some u∗∈⋀p−1(E∗) and relation (81) therefore implies ej∧z=0 for 1≤j≤n. It follows that in the expression z=∑HaHeH (where H runs through the set of subsets of {1,n} with p elements) all the coefficients aH are zero, whence z=0, contrary to the hypothesis.
The criterion of Proposition 16 is equivalent to writing conditions (81) when u∗ runs through a basis of ⋀p−1(E∗). In particular, suppose that E is of finite dimension n and let (ei)1≤i≤n be a basis of E. Conditions (81) are then equivalent to the conditions
(82−(J,H)) ⟨eJ∗,(eH∗⊥eI)∧z⟩=0 for all subsets J, H of
{1,n} such that
Card(J)=p+1 and
Card(H)=p−1. Now, if I and I' are two subsets of
{1,n} with
p elements, formulae (76) of no. 10 and multiplication table (20) of § 7, no. 8 show that
⟨eJ∗,⟨eH∗⊥eI⟩∧eI′⟩=0 unless there exists an
i∈{1,n} such that
I−H={i} and
J−I′={i}, in which case
⟨eJ∗,(eH∗⊥eI)∧eI′⟩=(−1)(p−1)(p−2)/2εi,J,H where
εi,J,H=ρ{i},Hρ{i},I′; it can then be said that for
i∈J∩CH,
εi,J,H is equal to
+1 if the number of element of J which are
<i and the number of elements of H which are
<i have the
same parity, and
−1 otherwise.
It follows immediately that if we write z=∑IaIeI, where I runs through the set of subsets of {1,n} with p elements, relation (82–(J, H)) is equivalent to the relation
i∈J∪CH∑εi,J,HaJ−{i}aH∪{i}=0.
Relations (84) are called Grassman’s relations; these are therefore necessary and sufficient conditions (when J describes the set of subsets with p+1 elements and H the set of subsets with p−1 elements of {1,n}) for an element z=0 of ⋀p(E) to be pure.
Note that relations (84) are not independent. For example, for n=4 and p=2, Grassmann’s relations reduce to the single relation
a12a34−a13a24+a14a23=0.
Let Dp(E) be the subset of ⋀p(E) consisting of the pure p-vectors; clearly Dp(E) is saturated with respect to the equivalence relation between u and v: “there exists λ∈K∗ such that v=λu” and two elements u,v of Dp(E) are equivalent under this relation if and only if the subspaces Mu and Mv of E which are associated with them are the same. Therefore we thus obtain a canonical bijection of the set of p-dimensional vector subspaces of E onto the image Gp(E) of Dp(E) in the projective space P(⋀p(E)) associated with ⋀p(E). The subset Gp(E) of P(⋀p(E)) is called the Grassmannian of index p of the vector space E. When E is finite-dimensional and (ei)1≤i≤n is a basis of E, the Grassmannian of index p is the set of points of P(⋀p(E)) for which a system of homogeneous coordinates (aI) (relative to the basis (eI) of ⋀p(E)) satisfies Grassmann’s relations (84).
When E=Kn, we sometimes write Gn,p(K) instead of Gp(Kn), so that Gn,1(K)=Pn−1(K). The mapping M↦M0, which associates with every p-dimensional subspace of Kn the orthogonal subspace in E∗ (identified with Kn under the choice of basis dual to the canonical basis of Kn) therefore defines a canonical bijection of Gn,p(K) onto Gn,n−p(K); Proposition 15 shows that this bijection is the restriction to Gn,p(K) of a canonical isomorphism of the projective space P(⋀p(Kn)) onto the projective space P(⋀n−p(Kn)).
Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.
Nothing.