Bourbaki

Proposition 13

Tag 0DSY, permanent. Cite it as [Bourbaki, Tag 0DSY].

Algebra, chapter X, § 2. Complexes de A-modules

There exists a unique k-antiderivation d:ΩA/k→ΩA/kd : \Omega_{A/k} \to \Omega_{A/k} of degree 1, square zero, which extends the derivation d0:A→ΩA/k1d^0 : A \to \Omega^1_{A/k}.

Let us prove the uniqueness of the antiderivation d. Since d∘d=0d \circ d = 0, one has for y,x1,…,xp∈Ay, x_1, \ldots, x_p \in A:

d(ydx1∧…∧dxp)=dy∧dx1∧…∧dxp. d(y dx_1 \wedge \ldots \wedge dx_p) = dy \wedge dx_1 \wedge \ldots \wedge dx_p .
The A-module ΩA/kp\Omega^p_{A/k} being generated by the elements dx1∧…∧dxpdx_1 \wedge \ldots \wedge dx_p, this proves the uniqueness of d.

To prove existence, it suffices to construct a kk-homomorphism d1:ΩA/k1→ΩA/k2d^1 : \Omega_{A/k}^1 \to \Omega_{A/k}^2 such that d1∘d0=0d^1 \circ d^0 = 0 and

d1(aω)=d0(a)∧ω+ad1(ω)for a∈A,ω∈ΩA/k1. d^1(a \omega) = d^0(a) \wedge \omega + a d^1(\omega) \quad \text{for } a \in A , \quad \omega \in \Omega_{A/k}^1 .
Indeed, it then follows from III, p. 128, prop. 14 (taking into account III, p. 118, remark 2) that there exists an antiderivation d:ΩA/k→ΩA/kd : \Omega_{A/k} \to \Omega_{A/k} which coincides with d0d^0 in degree 0 and with d1d^1 in degree 1. Since d0d^0 is zero on AA, the antiderivation dd is kk-linear; since d1∘d0=0d^1 \circ d^0 = 0, one has d∘d=0d \circ d = 0 since ΩA/k\Omega_{A/k} is generated as an AA-algebra by the elements d0ad^0 a for a∈Aa \in A.

To define d1d^1, let us recall (III, p. 133) that ΩA/k1\Omega_{A/k}^1 is equal to the AA-module J/J2\mathfrak{J}/\mathfrak{J}^2, where J\mathfrak{J} is the kernel of the multiplication m:A⊗kA→Am : A \otimes_k A \to A. Consider the kk-linear mapping u:A⊗kA→ΩA/k2u : A \otimes_k A \to \Omega_{A/k}^2 defined by u(x⊗y)=d0(y)∧d0(x)u(x \otimes y) = d^0(y) \wedge d^0(x). We have

u(ax⊗y−x⊗ay)=d0(y)∧d0(ax)−d0(ay)∧d0(x)=d0(xy)∧d0(a) u(ax \otimes y - x \otimes ay) = d^0(y) \wedge d^0(ax) - d^0(ay) \wedge d^0(x) = d^0(xy) \wedge d^0(a)
for x,yx, y and aa in AA, whence
u((a⊗1−1⊗a)ξ)=d0(m(ξ))∧d0(a),ξ∈A⊗kA,a∈A. u((a \otimes 1 - 1 \otimes a) \xi) = d^0(m(\xi)) \wedge d^0(a) , \quad \xi \in A \otimes_k A , \quad a \in A .
Since J\mathfrak{J} is generated as a left AA-module by the elements (a⊗1−1⊗a)(a \otimes 1 - 1 \otimes a) for a∈Aa \in A, we deduce that u(J2)=0u(\mathfrak{J}^2) = 0; consequently uu defines by restriction to J\mathfrak{J} and passing to the quotient a kk-linear mapping d1:J/J2→ΩA/k2d^1 : \mathfrak{J}/\mathfrak{J}^2 \to \Omega_{A/k}^2.

By setting ξ=b⊗1\xi = b \otimes 1 in (12), with b∈Ab \in A, we obtain d1(bd0(a))=d0(b)∧d0(a)d^1(b d^0(a)) = d^0(b) \wedge d^0(a); it follows that d1∘d0=0d^1 \circ d^0 = 0 and that d1(cω)=d0(c)∧ω+cd1(ω)d^1(c \omega) = d^0(c) \wedge \omega + c d^1(\omega) for c∈Ac \in A and ω=bd0(a)\omega = b d^0(a). Since ΩA/k1\Omega_{A/k}^1 is generated as a kk-module by the elements bd0(a)b d^0(a), for aa and bb in AA, formula (11) is satisfied for all ω∈ΩA/k\omega \in \Omega_{A/k}, which completes the proof of the proposition.

One sometimes says that the elements ω∈ΩA/kp\omega \in \Omega_{A/k}^p are the exterior differential forms of degree pp of AA over kk, and that the antiderivation dd is the exterior differential of ΩA/k\Omega_{A/k}; the complex (ΩA/k,d)(\Omega_{A/k}, d) is called the de Rham complex of A over k, and its homology is the de Rham cohomology of A over k.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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