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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedaudited 2026-09-27
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Relative differentials commute with scheme base change

Statement

Let X→S be a morphism of schemes and let S′→S be a morphism, with fibre product X′=X×SS′,g ⁣:X′⟶X,X′⟶S′. Then the canonical map g∗ΩX/S⟶ΩX′/S′,1⊗dX/S(a)⟼dX′/S′(a∘g), is an isomorphism of OX′-modules. It is natural in the base-change data and compatible with the universal derivations of X/S and X′/S′; no flatness, finiteness, separatedness or tor-independence hypothesis is imposed on S′→S or on X→S.

Facts & Assumptions

Given: Morphisms of schemes X→S and S′→S, with fibre product X′=X×SS′ and projections g ⁣:X′→X, X′→S′.

[F1]

Kähler differentials commute with scalar base change: for ring maps A→B and A→A′ with B′=B⊗AA′, the canonical B′-linear map ΩB/A⊗BB′→ΩB′/A′, db⊗a′↦a′d(b⊗1), is an isomorphism.

[F2]

Affine fibre products are spectra of tensor products: for affine opens U=Spec⁡B⊆X over V=Spec⁡A⊆S and W=Spec⁡A′⊆S′ over V, the open subscheme U×VW⊆X′ is affine with ring B⊗AA′.

[F3]

Sheaf of relative Kähler differentials: ΩX/S carries the universal S-derivation dX/S, an S-derivation of OX kills the image of the structure map from OS, and ΩX′/S′ is defined analogously.

[F4]

Universal property of relative differential sheaves: composition with dX/S is a natural bijection Hom⁡OX(ΩX/S,F)≅Der⁡S(OX,F) for every OX-module F.

[F5]

Pullback of modules is left adjoint to pushforward: there is a natural bijection Hom⁡OX′(g∗G,F)≅Hom⁡OX(G,g∗F), and the map corresponding to u sends 1⊗s to u(s).

[F6]

Pullback of a module along a morphism of ringed spaces: g∗G=OX′⊗g−1OXg−1G, and a local section a of OX acts on g∗G as a∘g.

[F7]

Affine charts recover the algebraic module of differentials and The stalk of a presheaf at a point: on an affine chart, ΩX/S is the sheaf attached to the relevant algebraic module with the restriction maps given by localization, and stalks are filtered colimits of sections over basic opens.

Proof

technique · direct
1.1

The canonical map. The composite D ⁣:OX→g∗OX′→g∗dX′/S′g∗ΩX′/S′ is an S-derivation of OX into the OX-module g∗ΩX′/S′: it is additive, satisfies Leibniz for the OX-module structure transported along g♯, and kills the image of OS, because that image is mapped into the image of the OS′-structure of X′, which dX′/S′ annihilates by [F3]. By [F4] there is a unique OX-linear u ⁣:ΩX/S→g∗ΩX′/S′ with u(dX/S(a))=dX′/S′(a∘g), and by [F5] there is a unique OX′-linear map γ ⁣:g∗ΩX/S→ΩX′/S′ sending 1⊗dX/S(a) to dX′/S′(a∘g).

F3F4F5F6
2.1

Affine charts compute γ. Let x′∈X′ have image x∈X and s∈S, and choose an affine open V=Spec⁡A⊆S containing s; then choose an affine open U=Spec⁡B⊆X containing x with image in V and an affine open W=Spec⁡A′⊆S′ containing the image of x′ with image in V. By [F2], U′:=U×VW=Spec⁡B′ for B′=B⊗AA′ is an open affine neighbourhood of x′. By [F7], ΩX/S∣U and ΩX′/S′∣U′ are attached to ΩB/A and ΩB′/A′. If x′ corresponds to p′⊆B′ and x to p=p′∩B, the pullback definition [F6] and stalk construction [F7] give (g∗ΩX/S)x′≅(ΩB/A)p⊗BpBp′′≅(B′⊗BΩB/A)p′. Hence the pullback is the sheaf attached to B′⊗BΩB/A on U′. The map γ sends 1⊗db to d(b⊗1) by step 1.1, so on these stalks it is the localisation of the canonical isomorphism of [F1].

F1F2F6F7step 1.1
3.1

γ is an isomorphism. Every point x′∈X′ lies in a chart U′ as in step 2.1, on which γ∣U′ is the isomorphism of [F1]; a morphism of sheaves whose restriction to each member of an open cover is an isomorphism is an isomorphism (equivalently, its stalk maps are isomorphisms), and forming stalks of the sheaves attached to B′-modules at points of U′ is compatible with the identifications of step 2.1. Hence γ is an isomorphism of OX′-modules, with the asserted description on generators.

F1step 2.1
4.1

Naturality and hypotheses. The map γ was produced from the universal properties of [F4] and the adjunction [F5] applied to the given morphisms S′→S and X→S; replacing the base-change data by a morphism of squares replaces γ by the corresponding pullback of γ, and on affine charts this is the naturality statement of [F1]. Only the existence of the fibre product and the affine descriptions of Ω were used, so no flatness, finiteness, separatedness or tor-independence hypothesis enters.

F1F4F5step 2.1step 3.1∎

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