Entrywise Formula for Partial Symmetrization
ProvedFunctionalInequalities.KLS.LogConcave.PoissonIterate.symmetrize_apply_comp_cast_readableLet with , let be an -index coordinate tensor over an -element coordinate space, and let . Then the entry of the symmetrization over the first positions is the average over permutations of those positions, while the last positions remain fixed:
The equality includes the necessary cast from the equality and is an entrywise coordinate identity. It is used to expand symmetrized Taylor fields.
Original Lean declaration header
Within namespace FunctionalInequalities.KLS.LogConcave.PoissonIterate. Shown in its original module context. Proof omitted.
theorem symmetrize_apply_comp_cast {n N q r : ℕ} (h : N = q + r) (A : Coord n N)
(J : Fin (q + r) → Fin n) :
symmetrize n N q A (J ∘ Fin.cast h) =
(q.factorial : ℝ)⁻¹ * ∑ τ : Equiv.Perm (Fin q),
A (Fin.append (J ∘ Fin.castAdd r ∘ τ) (J ∘ Fin.natAdd q) ∘ Fin.cast h)
Module navigation
Module: KLS/BKL/PoissonIterate/Taylor.
Definition modules: Analysis/Tensor/Coordinate.
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Source excerpt, lines 201–205 · Frozen source 408915f.
import Definitions.Def_KLSModular_FunctionalInequalities_KLS_BKL_PoissonIterate_Taylor open FunctionalInequalities.Analysis.Tensor
theorem FunctionalInequalities.KLS.LogConcave.PoissonIterate.symmetrize_apply_comp_cast_readable {n N q r : ℕ} (h : N = q + r) (A : Coord n N)
(J : Fin (q + r) → Fin n) :
symmetrize n N q A (J ∘ Fin.cast h) =
(q.factorial : ℝ)⁻¹ * ∑ τ : Equiv.Perm (Fin q),
A (Fin.append (J ∘ Fin.castAdd r ∘ τ) (J ∘ Fin.natAdd q) ∘ Fin.cast h) := by sorry