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Rank-three alternating exterior class

PDF p. 17: Proof of Corollary 6.10, definition of beta

Definition

Assume the Axiom of Choice and the suitable universes used in the vector-bundle classes definition. Let X be a quasi-compact, quasi-separated scheme and let E be a rank-three vector bundle on X: that is, a locally free OX-module locally isomorphic to OX3. Write K0(X)=π0K(Perf⁡(X)) for the supplied degree-zero perfect K-theory group, and write [V] for the class in it of a vector bundle V viewed as a complex in degree zero.

The rank-three alternating exterior class of E is β(E)=[OX]−[E]+[Λ2E]−[det⁡E]∈K0(X). Here ΛiE is the ith exterior power and det⁡E=Λ3E. Equivalently, in the functional convention, define λ−1(E):=∑i=03(−1)i[ΛiE]; then β(E)=λ−1(E). This notation applies the alternating exterior-power expression to the bundle E; no extension to arbitrary virtual classes is asserted.

Facts & Assumptions

Given: A quasi-compact, quasi-separated scheme X, a rank-three vector bundle E, the Axiom of Choice and suitable universes as above.

Goal: Justify that the displayed expression defines an isomorphism-invariant element of K0(X) and equals the stated alternating sum.

[F1]

For such X, the supplied K0(X) is an abelian group, and a vector bundle V has an isomorphism-invariant class [V] in it; its unit is [OX]. Isomorphism classes of vector bundles

[F2]

Exterior powers of a rank-three bundle are vector bundles, functorial in the bundle; Λ0E is canonically OX, det⁡E=Λ3E, and ΛiE=0 for i>3. Exterior powers and determinant of an algebraic bundle

[F3]

The Axiom of Choice is assumed for the supplied perfect K-theory construction underlying the classes in [F1], with the same universe conventions as that supplier. This is the inherited use in step 1.1; the finite alternating-sum calculation requires no additional choice. The Axiom of Choice Isomorphism classes of vector bundles

Justification

1.1 By [F2], OX, E, Λ2E and det⁡E are vector bundles. Their classes exist in the abelian group K0(X) by [F1], so their indicated sum and differences define an element of that group. An isomorphism E≅E′ induces isomorphisms of the corresponding exterior powers by functoriality; consequently [F1] gives β(E)=β(E′). [given, F1, F2, F3]

2.1 Expanding the four terms in the defining sum for λ−1(E) and using Λ0E≅OX and Λ3E=det⁡E gives precisely the displayed formula for β(E). The higher exterior powers vanish, so the same expression is the full finite alternating exterior-power sum. [F2, step 1.1, algebra] ∎

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