(tensor algebra)
Let \(A\) be a commutative ring and let \(M\) be an \(A\)-module. The tensor algebra is the unital associative \(A\)-algebra \[ T^\bullet_A(M)\coloneqq\bigoplus_{n\ge0}T_A^n(M),\qquad T_A^0(M)=A,\qquad T_A^n(M)=M^{\otimes_A n}\quad(n>0), \] with multiplication given by concatenation of elementary tensors. For every unital associative \(A\)-algebra \(B\), an \(A\)-linear map \(M\to B\) extends uniquely to an \(A\)-algebra homomorphism \(T_A^\bullet(M)\to B\).
(symmetric algebra)
The symmetric algebra \(\Sym_A^\bullet(M)\) is the quotient of \(T_A^\bullet(M)\) by the two-sided ideal generated by \(m\otimes n-n\otimes m\), for \(m,n\in M\). Its degree-\(q\) component is the symmetric power \(\Sym_A^q(M)\). For every commutative \(A\)-algebra \(B\), an \(A\)-linear map \(M\to B\) extends uniquely to an \(A\)-algebra homomorphism \(\Sym_A^\bullet(M)\to B\).
(exterior algebra)
The exterior algebra \(\bigwedge_A^\bullet M\) is the quotient of \(T_A^\bullet(M)\) by the two-sided ideal generated by \(m\otimes m\), for \(m\in M\). Its degree-\(q\) component is the exterior power \(\bigwedge_A^q M\). For every unital associative \(A\)-algebra \(B\), an \(A\)-linear map \(\phi:M\to B\) with \(\phi(m)^2=0\) for all \(m\in M\) extends uniquely to an \(A\)-algebra homomorphism \(\bigwedge_A^\bullet M\to B\).
For integers \(m\ge1\) and \(q\ge0\) and a free module \(M\) with ordered basis \(e_1,\ldots,e_m\), the degree-\(q\) tensor, symmetric, and exterior powers have bases consisting of all length-\(q\) words, the degree-\(q\) monomials, and the increasing length-\(q\) wedges, respectively. Their ranks are \(m^q\), \(\binom{m+q-1}{q}\), and \(\binom m q\). In degree zero all three modules are \(A\). For \(M=0\), every positive-degree component is zero [@Har10a, Exercise II.5.16(a)].
(A commutative tensor algebra)
For \(M=Ae\) free of rank one, \(T_A^q(M)\) has basis \(e^{\otimes q}\) and concatenation gives \(e^{\otimes p}e^{\otimes q}=e^{\otimes(p+q)}\). Hence \(T_A^\bullet(Ae)\cong A[t]\), with \(e\) corresponding to \(t\). Thus a tensor algebra need not be noncommutative.
For homogeneous \(u\in\bigwedge_A^p M\) and \(v\in\bigwedge_A^q M\), \[ u\wedge v=(-1)^{pq}v\wedge u. \] The defining square relations give \(m\wedge n=-n\wedge m\) by expanding \((m+n)\wedge(m+n)=0\); moving \(p\) factors past \(q\) factors proves the formula, and linearity extends it to homogeneous sums.
(Tensor operations on sheaves)
For a sheaf \(\mcf\) of modules on a ringed space \((X,\OO_X)\), its tensor, symmetric, and exterior algebras are the sheafifications of the presheaves assigning the corresponding \(\OO_X(U)\)-algebra to \(\mcf(U)\) on each open set \(U\). Their degree-\(q\) components are denoted \(T^q(\mcf)\), \(S^q(\mcf)=\Sym^q(\mcf)\), and \(\bigwedge^q\mcf\) [@Har10a, Exercise II.5.16].
If \(\mcf\) is quasi-coherent and \(\mcf|_{\Spec A}\cong\widetilde M\), then \[ (\bigwedge^q\mcf)|_{\Spec A}\cong\widetilde{\bigwedge_A^q M}, \] and the corresponding identities hold for tensor and symmetric powers. These identities follow from compatibility of tensor products and their defining quotients with localization [@Har10a, Propositions II.5.2 and II.5.7, Exercise II.5.16(e)].
For a locally free sheaf \(\mcf\) of finite rank \(m\), its determinant is \(\det\mcf=\bigwedge^m\mcf\). For a smooth \(m\)-dimensional variety over a field \(k\), this gives the canonical invertible sheaf \(\omega_X=\bigwedge^m\Omega_{X/k}\) [@Har10a, Chapter II, §8]. For a locally free sheaf \(\mce\) of finite rank on a scheme \(X\), the projective bundle in the quotient convention is \(\PP(\mce)=\operatorname{Proj}_X\Sym^\bullet\mce\) [@Har10a, Chapter II, §7].
Dependencies
D-DEFGRRNGGraded rings, homogeneous ideals, and the irrelevant idealusesD-DEFTENSThe tensor product of modules, and extension of scalarsuses