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Projective volume trace duality for perfect complexes under derived base change

Statement

Assume the Axiom of Choice. Let k be a field, let X be a smooth projective k-scheme of pure dimension d, and choose an isomorphism nu from OX to ωX, where ωX is the determinant of the rank-d sheaf of differentials. Let tX be the normalized Serre trace on Hd(X,ωX), and let E be a finite locally free OX-module. Then the trace and evaluation pairing induces a quasi-isomorphism RΓ(X,E)→RHom⁡k(RΓ(X,E dual),k)[−d]. Moreover, for every connective derived commutative k-algebra A, write XA=X × Spec(A) for the derived base change. Derived sections CA(P)=R Γ(XA,P) are perfect A-modules for every perfect P, and commute with every further derived scalar extension A -> A′. The base-changed trace induces a quasi-isomorphism CA(P)→RHom⁡A(CA(P dual),A)[−d] for every such P. The structure sheaf is compact in QCoh(XA). Thus in characteristic zero the normalized volume trace supplies the full geometric orientation, including its derived-base-change condition, not only its vector-bundle restriction.

For a finite locally free E over k, equivalently, for every integer q the pairing Hq(X,E) x Hd−q(X,E dual) -> k obtained by evaluation, cup product, nu, and tX is perfect.

Facts & Assumptions

Given: A field k, a smooth projective pure d-dimensional k-scheme X, the chosen volume isomorphism nu: OX -> ωX, the normalized trace tX, a finite locally free OX-module E, and the Axiom of Choice as assumed by both pinned suppliers. Use cohomological shifts K[r]^j=K^(j+r).

[F1]

Dualizing line bundle and trace datum of a smooth projective variety: ωX is det ΩX/k1; a normalized trace tX is fixed, and its normalization is independent of the projective-space model used to define it.

[F2]

Serre duality for locally free sheaves on a smooth projective variety: for finite locally free E, cup product, contraction with E dual, and tX give perfect finite-dimensional pairings Hq(X,E) x Hd−q(X,E dual tensor ωX) -> k for 0≤q≤d; the cohomology groups vanish outside this range.

[A1]

The Axiom of Choice: adopt the Axiom of Choice; the cited trace and Serre-duality suppliers explicitly assume it.

[F3]

A finite sum of ample powers generates perfect complexes gives the coordinate Koszul generator, finite affine Čech localization, and the semifree tensor–Hom and compact-to-finite-cell arguments for the Noetherian discrete projective case. The extension of these explicit arguments to XA is given below, rather than assuming its Statement for a derived base.

[F4]

Cech cohomology computes quasi-coherent cohomology on a separated scheme gives the affine Čech computation for quasi-coherent sheaves. The bounded Čech direction extends it to derived modules as below.

Proof

1.1givenF1F2A1algebra

The isomorphism nu identifies E dual tensor ωX with E dual. Under this identification, the pairing in [F2] is exactly evaluation E tensor E dual -> OX, followed by cup product, nu: OX -> ωX, and tX. Thus its perfectness applies to the pairing in the Statement for every 0≤q≤d.

1.2givenF3F4A1construct

Choose a projective embedding X↪Pkr, put M=OX(1) and G=⨁j=0rM−j. Let Ua be its coordinate affine cover. For any connective derived k-algebra A, the base-changed intersections are derived affines with algebras O(UJ)⊗kLA. Their quasi-coherent derived modules are modules over these algebras; restrictions are derived localizations. Derived sections on XA are computed by the finite ordered Čech total complex on this cover. Indeed the augmented sheaf Čech complex has the contraction inserting an index containing the point. On each derived affine the module description makes sections exact in the stable sense. Thus this bounded Čech resolution computes derived sections on arbitrary modules; only finitely many Čech degrees occur, so totalization uses finite limits and no unbounded convergence assertion. It commutes with coproducts and filtered colimits. A perfect P is locally a finite-cell retract, so RHom⁡(P,−)=CA(P∨⊗−) preserves coproducts. In particular GA and OXA are compact.

2.1givenF2step 1.1algebra

Put C=RΓ(X,E) and D=RΓ(X,E∨). Since k is a field, Hom⁡k(−,k) is exact; applying it to cycles and boundaries gives naturally Hq(RHom⁡k(D,k)[−d])=Hom⁡k(Hd−q(D),k) under the stated shift convention. The morphism induced by evaluation, cup product, ν, and tX therefore induces on Hq exactly the perfect pairing of 1.1.

2.2F3F4A1step 1.2constructalgebra

The coordinate Koszul complexes remain locally contracted after derived scalar change: on Ua the section sa is still a unit, and insertion of sa−1 is the same contracting homotopy. Their finite cones show that all integral powers of MA lie in the thick closure of GA. If RHom⁡(GA,K)=0, consequently CA(K⊗MAn)=0 for every integer n. The filtered colimit under multiplication by sa identifies with sections on Ua,A, because on every affine chart it is precisely module localization by sa, and filtered colimits commute with the finite Čech totalization of step 1.2. Thus K restricts to zero on every derived affine Ua,A and is zero. This proves generation for arbitrary quasi-coherent derived modules, including unbounded ones. Finally repeat the actual tensor–Hom construction of [F3] with BA=RHom⁡(GA,GA): on semifree modules its unit is an equivalence on BA, then on sums, cones and sequential homotopy colimits; its counit's cone is killed by RHom⁡(GA,−) and hence zero by the detection just proved. This gives D(BA)≃QCoh⁡(XA). The compact-to-finite-cell argument in [F3] applies to every dg algebra, regardless of boundedness: a finite set of semifree generators has a finite differential closure because attachment stages decrease. A compact module is a retract of a finite cell submodule. Hence every perfect P on XA, compact by step 1.2, lies in the finite sum, shift, cone and retract closure of GA. No Noetherianity or finite amplitude of A has been imposed.

3.1F2step 2.1algebra

For q outside [0,d], both source and target cohomology in degree q vanish by [F2] and the displayed derived-dual formula. Hence the morphism induces an isomorphism on cohomology in every degree. A morphism of complexes is a quasi-isomorphism precisely when it induces such isomorphisms, proving its vector-bundle assertion.

3.2F2F3F4A1step 1.2step 2.2algebra

For every vector bundle V on X the same affine Čech complex gives naturally CA(VA)≃Ck(V)⊗kLA. A finite number of Čech terms is involved, and on each intersection this is the module scalar-extension identity. By [F2], Ck(V) has bounded finite-dimensional cohomology and is therefore perfect over k: split cycles and boundaries over the field, leaving a finite-dimensional cohomology complex. It follows that CA(VA) is perfect over A. For a map A→A′ the canonical comparison CA(P)⊗ALA′→CA′(P⊗ALA′) is an equivalence for every summand of GA by this formula. Both its sides are exact functors of P and preserve retracts. Step 2.2 proves the comparison for every perfect P. The same finite-closure argument proves perfection of CA(P). This proves all required compactness, finiteness and base-change assertions.

4.1F1F2F3F4A1step 3.1step 2.2step 3.2algebra∎

Construct the cap transformation by the evaluation map P⊗P∨→OXA, the Čech cup product and the scalar extension of the normalized trace of 1.1. These maps are natural, with the cohomological tensor signs, and commute with further scalar change by the very affine restriction and tensor maps of 3.2. For P=VA from a vector bundle on X, its cap map is the scalar extension of 1.1–3.1. Indeed Ck(V∨) is perfect, so the canonical dual base-change map RHom⁡k(Ck(V∨),k)⊗kLA→RHom⁡A(Ck(V∨)⊗kLA,A) is an equivalence, checked first on finite-dimensional shifts of k and then on finite cones and retracts. Thus the cap is an equivalence on each summand of GA. As functors of P, both CA(P) and RHom⁡A(CA(P∨),A)[−d] are exact and preserve finite sums and retracts; the second is covariant because it dualizes twice. Naturality gives a map of exact triangles, so two cap equivalences force the third by the cohomology long exact sequence. Equivalences also pass to shifts and retracts. Step 2.2 therefore proves the cap equivalence for every perfect P. This proves the claimed orientation at every connective derived base, with its actual trace and evaluation maps, and retains the original vector-bundle pairing as its restriction. For X=∅ all module categories and cap maps are zero; for d=0 the argument uses the empty exterior power and the same trace, without an intermediate-degree assumption.

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