The source slope cutoff of display (14.1) #
The phase-cut torsion pair is convenient for slicing arguments, while display
(14.1) of arXiv:1902.08184v4 is parametrized by a finite weak slope
b : ℝ. This module supplies the exact adapter.
The normalized phase of the cutoff is
slopeCutPhase b = arctan b / pi + 1 / 2.
For a nonzero heart object, muPlus and muMinus are the slopes of the
nonzero endpoint factors of a slicing HN filtration. Their normalized phases
are the intrinsic slicing endpoints phiPlus and phiMinus; consequently
the paper's classes {muMinus > b} and {muPlus <= b} are exactly
P((slopeCutPhase b, 1]) and P((0, slopeCutPhase b]).
On a nonzero slicing-semistable heart object, the normalized weak slope
recovers its slicing phase, including the phase-1 boundary.
A slicing HN filtration whose first and last factors are nonzero. It is used only to name the source extremal slopes; their phase normalizations are proved independent of this choice below.
- filtration : HNFiltration C sigma.slicing.P E
The chosen slicing HN filtration.
The filtration has at least one factor.
- first_nonzero : ¬Limits.IsZero (self.filtration.triangle ⟨0, ⋯⟩).obj₃
Its largest-phase endpoint factor is nonzero.
- last_nonzero : ¬Limits.IsZero (self.filtration.triangle ⟨self.filtration.n - 1, ⋯⟩).obj₃
Its smallest-phase endpoint factor is nonzero.
Instances For
Choose an HN filtration with nonzero endpoint factors.
Equations
- sigma.extremalHNData E hE = { filtration := Classical.choose ⋯, n_pos := ⋯, first_nonzero := ⋯, last_nonzero := ⋯ }
Instances For
The maximal HN slope muPlus of a nonzero heart object.
Equations
- sigma.muPlus E hE = sigma.weakStabilityFunctionOnHeart.slope ((sigma.extremalHNData E hE).filtration.triangle ⟨0, ⋯⟩).obj₃
Instances For
The minimal HN slope muMinus of a nonzero heart object.
Equations
- sigma.muMinus E hE = sigma.weakStabilityFunctionOnHeart.slope ((sigma.extremalHNData E hE).filtration.triangle ⟨(sigma.extremalHNData E hE).filtration.n - 1, ⋯⟩).obj₃
Instances For
The normalized phase of muPlus is the intrinsic largest slicing
phase.
The normalized phase of muMinus is the intrinsic smallest slicing
phase.
Convert a finite weak-slope cutoff to the normalized phase interval.
Equations
Instances For
The source inequality muMinus(E) > b is the strict lower phase
bound at slopeCutPhase b.
The source inequality muPlus(E) <= b is the upper phase bound at
slopeCutPhase b.
The source torsion class {E | muMinus(E) > b}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The source torsion-free class {E | muPlus(E) <= b}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The torsion pair of display (14.1), parametrized by its real slope cutoff.
Equations
Instances For
The exact source-slope version of the tilted-heart identification in display (14.1).