Ambient weak Harder--Narasimhan filtrations from a bounded heart #
This file extends weak HN filtrations from the heart of a bounded
t-structure to every ambient object. The construction follows the canonical
t-cohomological filtration. An object with amplitude [b, a] receives an HN
tower whose phases lie in (-a, 1-b].
The key point is strict separation between adjacent cohomological degrees. A
pure degree-a object has phases in (-a, 1-a], while the truncation below
degree a has phases strictly above 1-a. The generic Postnikov-splicing
operation can therefore concatenate their HN towers across the truncation
triangle.
Shift an HN filtration for an induced ambient weak phase family by an
integer. This is the non-circular analogue of HNFiltration.shiftHN: it uses
the shift law already proved directly for ambientPhasePredicate, before a
slicing has been assembled.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Heart-level HN existence supplies an ambient HN tower whose phases lie in
the standard interval (0, 1]. Recording the bounds together with the tower
avoids making later amplitude arguments depend on a particular choice.
A pure object concentrated in t-degree a has an ambient weak HN tower
with phases in (-a, 1-a].
Objects whose t-cohomology is supported in degrees [b, b+n] admit an
ambient weak HN tower with all phases in (-(b+n), 1-b]. The phase bounds
are the induction invariant that makes successive truncation triangles
strictly spliceable.
A bounded t-structure and weak HN filtrations on its heart determine HN filtrations for the integer-normalized ambient weak phase family on every object.
Global form of ambientHN_exists_of_bounded.
Boundedness of a heart tilt #
A Happel--Reiten--Smalø tilt of a bounded t-structure is bounded. In the
aisle convention used by HeartTorsionPair.tilt, an original amplitude
interval [b, a] becomes the tilted interval [b, a+1].