Let MM be a over a RR. Its symmetric algebra is

Sym⁡R(M)=TR(M)/⟨x⊗y−y⊗x:x,y∈M⟩,\operatorname{Sym}_R(M) =T_R(M)\big/\langle x\otimes y-y\otimes x:x,y\in M\rangle,

where TR(M)T_R(M) is the . It is a commutative RR-algebra graded by tensor degree, and its degree-one part receives the canonical map M→Sym⁡R(M)M\to\operatorname{Sym}_R(M).

Universal property

For every commutative unital RR-algebra AA and every RR-linear map f:M→Af:M\to A, there is a unique unital RR-algebra homomorphism

f~:Sym⁡R(M)⟶A\widetilde f:\operatorname{Sym}_R(M)\longrightarrow A

extending ff. This characterizes Sym⁡R(M)\operatorname{Sym}_R(M) as the free commutative RR-algebra on MM.

Examples

If MM is free with basis x1,…,xnx_1,\ldots,x_n, then

Sym⁡R(M)≅R[x1,…,xn].\operatorname{Sym}_R(M)\cong R[x_1,\ldots,x_n].

For a vector space VV, the degree-dd summand is its ddth symmetric power Sym⁡d(V)\operatorname{Sym}^d(V).

References
  1. Nicolas Bourbaki, Algebra I: Chapters 1–3, Springer, 1989. DOI record. Relevant: Chapter III, symmetric algebras.