Base-scheme linearity for external-product semiorthogonality #
This file refines the source tensor-closure hypothesis used by the
first-projection formula to the S-linearity appearing in Proposition 3.15.
It exposes both levels of the base action:
- compact objects of
Dqc(S), modeling the originalPerf(S)-linear decomposition; and - arbitrary objects of
Dqc(S), modeling its presentable quasicoherent extension.
Both act on Dqc(X) by genuine derived pullback along X → S, followed by
the K-flat source tensor. A projection coefficient pulled back from the
corresponding level on the base then gives the coefficient-local closure
required by the semiorthogonality argument.
The quasicoherent derived category of the base scheme.
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The compact objects of Dqc(S), modeling Perf(S) in this layer.
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For a fixed source object, the base-variable action functor: pull back
from S to X, then tensor on the right.
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The action of an arbitrary quasicoherent base object on Dqc(X): pull
it back along X → S, then tensor by it on the right.
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The action of a compact base object on Dqc(X): pull it back along
X → S, then tensor by it on the right.
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Paper-level S-linearity of the source semiorthogonal sequence: every
component is preserved by the action of every compact object of Dqc(S).
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Dqc(S)-linearity of the quasicoherent source components. This is the
presentable extension of S-linearity used when a projection coefficient on
the base is quasicoherent but not necessarily compact.
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Presentability data needed to extend the compact base action to all of
Dqc(S).
The base is generated from compact objects by coproducts and extensions, and for each fixed source object the action in the base variable is exact and preserves the relevant small coproducts.
Compact objects generate
Dqc(S)under coproducts and extensions.- actionCommShift (F : X.SourceDqc) : (dqcBaseActionInBase D Q pullBase F).CommShift ℤ
The action in the base variable commutes with shifts.
- actionTriangulated (F : X.SourceDqc) : (dqcBaseActionInBase D Q pullBase F).IsTriangulated
The action in the base variable is triangulated.
- actionCocontinuous (F : X.SourceDqc) : (dqcBaseActionInBase D Q pullBase F).PreservesSmallCoproducts
The action in the base variable preserves scheme-universe coproducts.
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Perf(S)-linearity extends to Dqc(S)-linearity when compact objects generate the base and the base action preserves triangles and coproducts.
Evidence that all source coefficients in a compact-fibre projection formula come by derived pullback from compact objects on the base scheme.
- baseCoefficient : T.CompactDqcFiber → T.CompactDqcFiber → ℤ → ℤ → CompactBaseDqc S
The compact object on
Srepresenting each source coefficient. - coefficientIso (Gi Gj : T.CompactDqcFiber) (a b : ℤ) : P.coefficient Gi Gj a b ≅ pullBase.functor.obj (self.baseCoefficient Gi Gj a b).obj
The projection coefficient is the pullback of its representing base object.
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Evidence that all projection-formula coefficients are pulled back from
quasicoherent objects on the base. Unlike BaseCoefficientData, this does
not require those objects to be compact.
- baseCoefficient : T.CompactDqcFiber → T.CompactDqcFiber → ℤ → ℤ → BaseDqc S
The quasicoherent object on
Srepresenting each coefficient. - coefficientIso (Gi Gj : T.CompactDqcFiber) (a b : ℤ) : P.coefficient Gi Gj a b ≅ pullBase.functor.obj (self.baseCoefficient Gi Gj a b)
The projection coefficient is the pullback of its representing base object.
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Compact base coefficients can be forgotten to quasicoherent base coefficients.
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Base coefficients and S-linearity imply the coefficient-local source
component preservation required by the projection formula.
Quasicoherent base coefficients and Dqc(S)-linearity imply the exact
coefficient-local preservation required by the projection formula.
Compact-fibre duality, a first-projection formula with base coefficients,
and S-linearity of the source sequence prove perfect-component
semiorthogonality after base change.
Compact-fibre duality, a first-projection formula with quasicoherent base
coefficients, and Dqc(S)-linearity of the source sequence prove
perfect-component semiorthogonality after base change.