Radical-power propagation in Iyama right ladders #
This file formalizes the annihilator-propagation calculation in Iyama, Tau-categories I, Lemma 6.4.1(1)(i). A weak-kernel right-ladder step moves an annihilator to the next rung up to its complementary term. Iteration and nilpotence then force one complementary composite to be nonzero in the corresponding radical power.
The explicit right-ladder step from Iyama, Section 3.2:
ZNext ⊞ U → YNext ⊞ ZPrev → YPrev,
with first-map matrix [[bNext, 0], [-g, h]] and second map
(f, bPrev).
Instances For
One weak-kernel right-ladder step propagates an annihilator across the
step, up to the complementary U-term.
This is the literal calculation
sPrev = sNext ≫ g + t ≫ h and sNext ≫ bNext = 0 in the proof of
Iyama 6.4.1(1)(i).
If an explicit right-ladder step is isomorphic to a right tau-sequence, then all three visible components of its first map belong to the chosen categorical radical ideal.
The next horizontal arrow in an explicit right-ladder step is radical.
Nonempty form of radicality of the next horizontal arrow.
Both connecting components in an explicit right-ladder step are radical.
Nonempty form matching the noncanonical mesh isomorphisms stored in
Iyama ladder data.
Family form aligned with the hypotheses of right-ladder radical-power propagation.
A right tau-sequence isomorphic to an explicit right-ladder step makes that step a weak-kernel complex.
The backwards composite of the first n right-ladder connecting maps.
Instances For
A chain of radical connecting maps has its length-n composite in the
nth ideal power.
The exact abstract output needed from every explicit right-ladder step.
Instances For
A family of explicit weak-kernel right-ladder steps supplies the abstract annihilator-propagation property.
Right tau-sequence models of all explicit ladder steps supply the annihilator propagation used in radical-power iteration.
If all complementary terms vanish after composing to the initial source, an initial annihilator propagates through every finite right-ladder prefix.
Radical-power propagation in the form used in Iyama 6.4.1(1)(i).
Starting from a nonzero annihilator, some complementary morphism
hᵢ ≫ gᵢ₋₁ ≫ ⋯ ≫ g₁ is nonzero. It automatically lies in the
corresponding radical power. Thus the hypothesis that every
Jⁱ(Uᵢ,Z₀) vanishes is incompatible with the initial nonzero
annihilator.