Cell-measure sum and joins of finite measurable partitions #
This file continues the measure-theoretic foundation for Kolmogorov–Sinai entropy started in
Oseledets.Entropy.Partition. It records that the cells of a MeasurePartition of a probability
space have μ-measures summing to 1, and introduces the cell family joinCells s t of the
join (common refinement) α ∨ β of two partitions, whose cells are the intersections
Aᵢ ∩ Bⱼ.
Following the Le Maître notes on the Kolmogorov–Sinai theorem, the join keeps all index pairs
(i, j) and allows null cells, so it is indexed by ι × κ.
Main definitions #
Oseledets.Entropy.joinCells: the family(i, j) ↦ s i ∩ t jof intersection cells of two families.
Main results #
Oseledets.Entropy.MeasurePartition.sum_toReal_measure_eq_one: the cell measures of a partition of a probability space sum to1.Oseledets.Entropy.entropy_le_log_card_partition: a partition intokcells has entropy at mostlog k.
References #
- François Le Maître, Notes on the Kolmogorov–Sinai theorem (2017), §1.
The μ-measures of the cells of a finite measurable partition of a probability space sum to
the total mass 1. The cells are measurable, pairwise almost-everywhere disjoint, and cover the
whole space, so finite additivity of μ over an a.e.-disjoint null-measurable family gives
∑ i, μ (cells i) = μ univ = 1.
Corollary of Proposition 1 (Le Maître). A finite measurable partition of a probability
space into k cells has Shannon entropy at most log k.
The cell family (i, j) ↦ s i ∩ t j underlying the join (common refinement) α ∨ β of two
families of cells s : ι → Set α and t : κ → Set α.
Equations
- Oseledets.Entropy.joinCells s t p = s p.1 ∩ t p.2