Order relations on slicings #
This file introduces the strict and weak relations on slicings used by both arXiv:2601.22994, Definition 2.1, and arXiv:2607.28411v1, Definition 3.12. They compare the phase of an object in the first slicing with the upper HN phase of the same object in the second slicing.
The source papers use different symbols for the same relations. The named predicates here keep that comparison independent of notation and of any central charge or geometric realization.
The strict order on slicings: every object of phase phi for s has all
HN phases strictly below phi for t.
This is P_s(phi) ⊆ P_t(< phi) in arXiv:2601.22994, Definition 2.1, and
P_s ≺ P_t in arXiv:2607.28411v1, Definition 3.12.
Equations
- CategoryTheory.Triangulated.Slicing.Precedes C s t = ∀ (phi : ℝ), s.P phi ≤ CategoryTheory.Triangulated.Slicing.ltProp C t phi
Instances For
The weak order on slicings: every object of phase phi for s has all
HN phases at most phi for t.
This is P_s(phi) ⊆ P_t(≤ phi) in both source papers.
Equations
- CategoryTheory.Triangulated.Slicing.PrecedesWeak C s t = ∀ (phi : ℝ), s.P phi ≤ CategoryTheory.Triangulated.Slicing.leProp C t phi
Instances For
Li's strict order notation, retained as a source-facing alias of the canonical strict slicing order.
Equations
Instances For
Li's weak order notation, retained as a source-facing alias of the canonical weak slicing order.
Equations
Instances For
The strict relation of arXiv:2601.22994, Definition 2.1, is exactly the strict relation of arXiv:2607.28411v1, Definition 3.12.
The weak relation of arXiv:2601.22994, Definition 2.1, is exactly the weak relation of arXiv:2607.28411v1, Definition 3.12.
The strict slicing order is equivalent to its upper-phase formulation on nonzero objects semistable for the left-hand slicing.
The weak slicing order is equivalent to its upper-phase formulation on nonzero objects semistable for the left-hand slicing.
A strict comparison is, in particular, a weak comparison.
The weak slicing order is reflexive.
Shifting all phases down by one strictly increases a slicing in the order:
P ≺ P[1], where P[1](phi) = P(phi + 1).
Shifting a slicing down by t subtracts t from the highest phase of a
nonzero object.
Shifting a slicing down by t subtracts t from the lowest phase of a
nonzero object.