Chapter III
Tensor Algebras, Exterior Algebras, Symmetric Algebras
Recall the exponential notation introduced in Chapter I, of which we shall make frequent use (I, § 7, no. 8):
Let (xλ)λ∈L be a family of pairwise permutable elements of a ring A; for every mapping α:L→N of finite support we shall write
xα=λ∈L∏xλα(λ).
If β is another mapping of L into N of finite support, α+β denotes the mapping
λ↦α(λ)+β(λ)
of L into N; with this law of composition the set N(L) of mappings of L into N of finite support is the free commutative monoid derived from L and
xαxβ=xα+β.
For all α∈N(L), we write ∣α∣=∑λ∈Lα(λ)∈N; then ∣α+β∣=∣α∣+∣β∣; ∣α∣ is called the order of the "multiindex" α. For all λ∈L, let δλ denote the element of N(L) such that δλ(λ)=1, δλ(μ)=0 for μ=λ (Kronecker index); the δλ for λ∈L are the only elements of N(L) of order 1. N(L) is given the ordering induced by the product ordering on NL, so that the relation α≤β is equivalent to "α(λ)≤β(λ) for all λ∈L"; then the multiindex λ↦β(λ)−α(λ) is denoted by β−α, so that it is the unique multiindex such that α+(β−α)=β. For all α∈N(L), there are only a finite number of multiindices β≤α; the δλ are the minimal elements of the set N(L)−{0}; the relation α≤β implies ∣α∣≤∣β∣ and if both α≤β and ∣α∣=∣β∣, then α=β.
Finally, we write α!=∏λ∈L(α(λ))!, which is meaningful since 0!=1.
From § 4 to § 8 inclusive, A denotes a commutative ring and, unless otherwise stated, the algebras considered are assumed to be associative and unital and the algebra homomorphisms are assumed to be unital.