Small-grid cycles and boundaries for the fully blocked grid differential #
This file computes the cycle and boundary submodules of the fully blocked grid differential in the already-proved zero-differential small-grid case.
Main results #
TauCeti.GridDiagram.fullyBlockedCycles_eq_top_of_le_twoandTauCeti.GridDiagram.fullyBlockedBoundaries_eq_bot_of_le_two: the small-grid computation.TauCeti.GridDiagram.natCard_fullyBlockedCycles_of_le_twoandTauCeti.GridDiagram.natCard_fullyBlockedBoundaries_of_le_two: the small-grid cardinalities.
References #
This supplies a prerequisite for TauCetiRoadmap/CombinatorialHeegaardFloer/README.md,
Lane G.3, "The complexes and ∂² = 0", and for the standing convention that grid complexes
compute on explicit small grids.
In grid size at most two, every chain is a cycle for the fully blocked differential.
In grid size at most two, the only boundary for the fully blocked differential is zero.
On every 2 × 2 grid, every chain is a cycle for the fully blocked differential.
On every 2 × 2 grid, the only boundary for the fully blocked differential is zero.
In grid size at most two, every chain is a fully blocked cycle.
In grid size at most two, a fully blocked boundary is exactly the zero chain.
On every 2 × 2 grid, every chain is a fully blocked cycle.
On every 2 × 2 grid, a fully blocked boundary is exactly the zero chain.
In grid size at most two, there are 2 ^ n! fully blocked cycles.
In grid size at most two, there is one fully blocked boundary.
Every 2 × 2 grid has four fully blocked cycles.
Every 2 × 2 grid has one fully blocked boundary.