The torsion pair of a weak stability function at a slope cutoff #
For a weak stability function W on an abelian category with the Harder--Narasimhan property,
and a cutoff μ₀ : WithTop ℝ, the two classes of WeakCutoff.lean
T μ₀ = {E | every weak HN slope of E exceeds μ₀} F μ₀ = {E | every one is at most μ₀}
are a TorsionPair. Both axioms are now proved:
hom_eq_zeroishom_eq_zero_of_mem_hnTors_of_mem_hnFree(#789) — the image of a map is a quotient of the source and a subobject of the target, soμMinus_le_of_epiandμPlus_le_of_monotrap its slopes in the empty interval(μ₀, μ₀];exists_shortExactisexists_shortExact_hnTors_hnFree(WeakSplitting.lean) — the HN chain cut at the index where its slopes crossμ₀.
What took so long, recorded because it is the interesting part #
The Hom-vanishing axiom ported from the strict theory almost verbatim in #789. The splitting
did not, and the obstruction was two levels below where it looked: not in Cutoff.lean and not
in the torsion-pair assembly, but in Uniqueness/SubobjectLattice.lean, whose
pullback_imageSubobject_eq and cokernelPullbackIso were proved from
semiClosedUpperHalfPlane_ne_zero — a nonzero object has nonzero charge. That is exactly the
implication weak stability drops, and it fails on exactly the object the surface case of
Bridgeland's Lemma 6.2 is about. Both statements are true in any abelian category;
CategoryTheory/SubobjectCorrespondence.lean proves them without a charge, WeakTail.lean
ports the truncation on top of them, and this file is what that unblocks.
Cutoff by slope, not by phase #
The strict pair (TorsionPair/StabilityFunction.lean) is cut by a phase β : ℝ. This one is
cut by a slope in WithTop ℝ, which is what lets a rank-zero object — slope ⊤, no phase at
all — sit in T μ₀ at every finite cutoff (WeakSlopeData.mem_hnTors_of_rank_zero, #801).
The torsion class at a weak slope cutoff, as an ObjectProperty.
Equations
- W.hnTorsProperty μ₀ E = (E ∈ W.hnTors μ₀)
Instances For
The torsion-free class at a weak slope cutoff, as an ObjectProperty.
Equations
- W.hnFreeProperty μ₀ E = (E ∈ W.hnFree μ₀)
Instances For
The two classes at a weak slope cutoff are a torsion pair.
Equations
- One or more equations did not get rendered due to their size.