K-flat fibre coefficients for base-change semiorthogonality #
This file makes the fibre object in the faithful-base-change argument
concrete. A K-flat resolution on T supplies the derived tensor on Dqc(T),
and compact duality chooses G⁺ right-adjoint to tensoring by each compact
fibre object G. The coefficient attached to Gi[a] and Gj[b] is then
(Gj ⊗ Gi⁺)[b - a].
The remaining comparison with the coefficient produced by the first projection formula is kept explicit. It is precisely the associativity, pullback/tensor, and duality coherence still missing from the current K-flat monoidal layer.
A K-flat construction of the derived tensor on Dqc(T).
- resolution : SchemeKFlatResolution (CategoryTheory.Over.left T)
A K-flat replacement on the fibre scheme.
- tensorQuasicoherent : self.resolution.ResolvedTensorPreservesQuasicoherentCohomology
Resolved tensor preserves quasicoherent cohomology.
Instances For
The derived tensor on Dqc(T) selected by the K-flat fibre data.
Equations
Instances For
Chosen compact duals for the actual K-flat tensor on Dqc(T).
The adjunction records that tensoring on the right by G⁺ is right adjoint
to tensoring on the right by G.
- dual : T.CompactDqcFiber → T.CompactDqcFiber
The chosen compact dual of a compact fibre object.
- adjunction (G : T.CompactDqcFiber) : K.derivedTensor.flip.obj G.obj ⊣ K.derivedTensor.flip.obj (self.dual G).obj
Tensor-duality adjunction for the chosen compact dual.
Instances For
The explicit fibre coefficient left by dualizing Gi[a] against
Gj[b]: tensor Gj by the chosen dual of Gi, then shift by b - a.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The target-side tensor coefficient obtained by pulling back the two compact fibre factors separately, tensoring them with the target K-flat tensor, and applying the shift left by compact duality.
This is the intermediate object at which the projection-formula comparison and the monoidality of fibre pullback meet.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Atomic comparisons underlying the explicit K-flat fibre coefficient.
The first isomorphism is the projection-formula/duality calculation on
X_T. The second isomorphism is the tensor compatibility of pullback from
T. Keeping them separate prevents either geometric theorem from being
hidden in the final coefficient comparison.
- projectionIso (Gi Gj : T.CompactDqcFiber) (a b : ℤ) : P.coefficient Gi Gj a b ≅ pushFst.functor.obj (D.pulledBackTensorCoefficient K V Gi Gj a b)
Projection formula and compact duality identify the source coefficient with the pushforward of the separately pulled-back tensor coefficient.
- pullbackTensorIso (Gi Gj : T.CompactDqcFiber) (a b : ℤ) : D.pulledBackTensorCoefficient K V Gi Gj a b ≅ D.pullSnd.functor.obj (V.coefficient Gi Gj a b)
Pullback from the fibre commutes with its K-flat tensor coefficient.
Instances For
The first-projection coefficient is represented by the explicit K-flat fibre tensor of the later factor with the dual of the earlier factor.
- coefficientIso (Gi Gj : T.CompactDqcFiber) (a b : ℤ) : P.coefficient Gi Gj a b ≅ pushFst.functor.obj (D.pullSnd.functor.obj (V.coefficient Gi Gj a b))
Comparison between the abstract projection coefficient and the pushforward of the explicit pulled-back fibre tensor coefficient.
Instances For
Forget the explicit tensor formula while retaining its fibre coefficient and comparison.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Compose the projection/duality comparison with monoidality of fibre pullback to obtain the coefficient comparison used by faithful base change.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The atomic K-flat comparisons also supply the fibre-coefficient datum consumed by the faithful-base-change argument.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The end-to-end semiorthogonality theorem with all three tensor operations and the base pullback pinned to K-flat constructions, and with faithful base change applied to the explicit dual fibre coefficient.
The end-to-end semiorthogonality theorem stated using the two atomic coherence comparisons rather than a bundled coefficient isomorphism.