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Anderson4D.DetParametrix.Paper41_Renorm.R322FiberTail

Canonical ambient tails of an R-322 extraction fibre #

ExtractionComplementFiberAt is naturally a pairing on the complement subtype. That representation is ideal for a single block split, but awkward for iteration because the next reduction step is formulated on the original ordered ambient carrier. This file gives the exact missing bridge:

No quotient and no multiplicity factor is introduced.

Tail extraction on the original ambient carrier #

theorem Anderson4D.extractionFiber_tail_extractAux_eq {m : ℕ} (κ : PartialPairing (Fin m)) (fuel : ℕ) (active : Finset (Fin m)) (h : ∃ (a : Fin m) (b : Fin m), IsRelFullyPaired κ active a b) (τ : ExtractionFiberAt κ fuel active) :
extractAux (↑τ) fuel (active \ selectedExtractionBlock κ active h) = extractAux κ fuel (active \ selectedExtractionBlock κ active h)

Equality of the complete nonempty extraction lists implies equality of their tails on the carrier left after the common first block is removed.

Canonical ambient representatives of complementary coordinates #

@[reducible, inline]
abbrev Anderson4D.CanonicalExtractionTailAt {m : ℕ} (κ : PartialPairing (Fin m)) (fuel : ℕ) (active : Finset (Fin m)) (h : ∃ (a : Fin m) (b : Fin m), IsRelFullyPaired κ active a b) :

Ambient members of the current extraction fibre whose exposed first primitive coordinate is the reference coordinate. Their remaining pairing is precisely the recursive tail data.

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    def Anderson4D.extractionComplementFiberEquivCanonicalTail {m : ℕ} (κ : PartialPairing (Fin m)) (fuel : ℕ) (active : Finset (Fin m)) (h : ∃ (a : Fin m) (b : Fin m), IsRelFullyPaired κ active a b) :

    The complement-subtype coordinate is exactly a canonical ambient tail. This is the complement-to-tail bridge needed to iterate the one-block factorization without changing the ambient ordered carrier.

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      theorem Anderson4D.CanonicalExtractionTailAt.tail_extractAux_eq {m : ℕ} (κ : PartialPairing (Fin m)) (fuel : ℕ) (active : Finset (Fin m)) (h : ∃ (a : Fin m) (b : Fin m), IsRelFullyPaired κ active a b) (τ : CanonicalExtractionTailAt κ fuel active h) :
      extractAux (↑↑τ) fuel (active \ selectedExtractionBlock κ active h) = extractAux κ fuel (active \ selectedExtractionBlock κ active h)

      Every canonical ambient tail has the correct next extraction on the shrunk active carrier.

      First block followed by an ambient recursive tail #

      def Anderson4D.extractionFiberEquivBlockCanonicalTail {m : ℕ} (κ : PartialPairing (Fin m)) (fuel : ℕ) (active : Finset (Fin m)) (h : ∃ (a : Fin m) (b : Fin m), IsRelFullyPaired κ active a b) :

      Exact one-step extraction-fibre equivalence whose second coordinate stays on the original ambient carrier and is ready for the next active set.

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        theorem Anderson4D.sum_extractionFiber_eq_sum_block_canonicalTail {m : ℕ} (κ : PartialPairing (Fin m)) (fuel : ℕ) (active : Finset (Fin m)) (h : ∃ (a : Fin m) (b : Fin m), IsRelFullyPaired κ active a b) {M : Type u_1} [AddCommMonoid M] (F : ExtractionFiberAt κ fuel active → M) :
        ∑ τ : ExtractionFiberAt κ fuel active, F τ = ∑ κB : ↥(primitiveFullPairings (residualBlockOrder (selectedExtractionBlock κ active h))), ∑ tail : CanonicalExtractionTailAt κ fuel active h, F ((extractionFiberEquivBlockCanonicalTail κ fuel active h).symm (κB, tail))

        Finite-sum form of extractionFiberEquivBlockCanonicalTail; it exposes one complete primitive coordinate and an ambient recursive tail with no cardinality loss.