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DerivedAlgGeo.CategoryTheory.Abelian.Stability.Weak.CutoffSlope

The weak cutoff bounds the object's own slope, not only its factors' slopes #

hnTors W μ₀ and hnFree W μ₀ are defined by the Harder--Narasimhan extrema μ⁻ and μ⁺. Every consumer that wants to read a cutoff against a charge needs the object's own slope instead, and the step between them is that W.slope E lies between μ⁻ and μ⁺.

This is CutoffPhase.lean for the weak, slope-indexed theory.

Why this is not the strict proof #

CutoffPhase.lean gets the strict statement from HNPolygon.lean's phase_le_first and last_le_phase, which read the HN filtration as a convex polygonal path in ℂ and cite ComplexPolygonalPath.arg_last_sub_zero_le_arg_first. That apparatus is arg-geometry on semiClosedUpperHalfPlane and does not survive the weakening: the charges here may be 0, where arg says nothing.

The weak statement instead falls straight out of the see-saw of WeakSlopeGeometry.lean, by induction along the chain. Each step adds one factor charge to the running total, and the see-saw traps the new slope between the factor's slope and the old total's — so μ⁺ is never exceeded above and the current factor's slope is never dropped below. No polygon, and no convexity argument.

One thing makes this easier than the strict case rather than harder: 0 ∈ closedUpperHalfPlane, so charge_mem_closedUpperHalfPlane holds for every object including the zero one, and the induction carries no nonvanishing side conditions. In the strict theory that membership fails at 0 and the bookkeeping is real.

The payoff #

lt_slope_of_mem_hnTors and slope_le_of_mem_hnFree are what a charge comparison consumes, and unlike their strict counterparts they carry no positive-rank hypothesis: a rank-zero object has slope ⊤, which is above every finite cutoff, so it needs no separate treatment. On the strict side that object has to be routed around through mem_hnTors_of_rank_zero instead.

The slope of a sum lies between the slopes of its summands. The two see-saws combined by le_total, in the form an induction over a filtration consumes.

Every object's charge lies in the closed upper half-plane, the zero object included: its charge is 0, which the closed half-plane contains and the semi-closed one does not. This is the hypothesis-free membership the strict theory cannot have.

Each chain step is a short exact sequence with the corresponding factor as its cokernel, so the charges add.

The running total of an HN filtration stays inside the slope range.

Induction along the chain. At k = 1 the term is the maximal destabilizing subobject, whose slope is μ⁺ exactly. Each further step adds the next factor, whose slope is below everything already accumulated, so the see-saw puts the new total between that factor's slope and the old total's.

The object's own slope does not exceed the highest HN slope.

The lowest HN slope does not exceed the object's own slope.

An object of the torsion class has slope strictly above the cutoff.

hnTors says every HN slope exceeds μ₀; this says the object's own does. The zero object is excluded because it has no filtration — hnTors admits it separately.

Unlike SlopeData.slopeOfPhase_lt_of_mem_hnTors, there is no positive-rank hypothesis: a rank-zero object has slope ⊤, above every finite cutoff, and is covered by the same statement.

An object of the torsion-free class has slope at most the cutoff.