Radical-power propagation in Iyama left ladders #
This is the categorical dual of the right-ladder calculation in Iyama, Tau-categories I, Lemma 6.4.1(1)(i). The explicit matrix is obtained by opposing the right-ladder matrix and then writing the biproducts back in the original category.
The explicit left-ladder step, dual to Iyama's right-ladder step:
YPrev → YNext ⊞ ZPrev → ZNext ⊞ U,
with first map (f, bPrev) and second-map matrix
[[bNext, -g], [0, h]].
Instances For
One weak-cokernel left-ladder step propagates a coannihilator across the
step, up to the complementary U-term.
This is the dual identity
sPrev = g ≫ sNext + h ≫ t with bNext ≫ sNext = 0.
If an explicit left-ladder step is isomorphic to a left tau-sequence, then all three visible components of its second map belong to the chosen categorical radical ideal.
The next horizontal arrow in an explicit left-ladder step is radical.
Nonempty form of radicality of the next horizontal arrow.
Both connecting components in an explicit left-ladder step are radical.
Nonempty form matching noncanonical mesh isomorphisms.
Family form aligned with left-ladder radical-power propagation.
A left tau-sequence isomorphic to an explicit left-ladder step makes that step a weak-cokernel complex.
The forwards composite of the first n left-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 left-ladder step.
Instances For
A family of explicit weak-cokernel left-ladder steps supplies the abstract coannihilator-propagation property.
Left tau-sequence models of all explicit ladder steps supply the coannihilator propagation used in radical-power iteration.
If all complementary terms vanish after composing from the initial target, an initial coannihilator propagates through every finite left-ladder prefix.
Radical-power propagation dual to Iyama 6.4.1(1)(i).
Starting from a nonzero coannihilator, some complementary morphism
g₁ ≫ ⋯ ≫ gᵢ₋₁ ≫ hᵢ is nonzero and lies in the corresponding
radical power.