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DerivedAlgGeo.CategoryTheory.Triangulated.StabilityCondition.Weak.Heart.Equivalence

Weak stability on the heart of a slicing #

This file is the semistable-object part of the weak heart--slicing correspondence from Lemma 14.4 of arXiv:1902.08184v4. A weak prestability condition restricts to a weak stability function on its slicing heart. The only new boundary case relative to the ordinary construction is phase 1: compatibility permits a zero radius there, and therefore the induced heart charge lands on the closed negative real ray.

The main declarations are:

The analytic proof splits at phase 1. Below 1, every nonzero HN factor has strictly positive radius and the ordinary argument-convexity API applies. At phase 1, additivity and the closed half-plane force both ends of every heart short exact sequence to have zero imaginary part, hence slope +infinity.

Restrict a weak prestability condition to its slicing heart.

Equations
Instances For

    A heart subobject of a slicing-semistable object has top HN phase at most the phase of the ambient object. The subobject is presented by a distinguished triangle whose three vertices lie in the slicing heart.

    Below the boundary phase, the induced weak charge is nonzero and its argument is bounded above by the largest slicing HN phase.

    If the induced weak charge has positive imaginary part, its argument is bounded below by the smallest slicing HN phase. Zero-charge phase-1 factors are discarded from the sum; positive imaginary part guarantees that at least one charged factor remains.

    Slicing ray membership in (0,1] implies slope semistability for the induced weak stability function on the slicing heart.

    A nonzero heart object that is slope-semistable for the induced weak stability function lies in the slicing at its intrinsic top phase.

    For nonzero heart objects, slicing semistability and semistability for the induced weak stability function are equivalent.