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LeanPool.RegtsSevenster.RS.Novel.Coordinates.StdTransport

The model transport #

Given the strand identification of the standard model, the iterated identification of the monoidal powers: stdToOmega assembles copies of the strand map left-nested through the structure maps of the fibre functor, stdFromOmega disassembles, and the two are mutually inverse whenever the strand maps are.

noncomputable def RS.stdToOmega {R : ℕ} (f : EdgeRankParameter R) (P : DelignePackage (SkeinObj f)) {k ℓ : ℕ} (e : stdSuperPair k ℓ ⟶ P.ω.obj { arity := 1 }) (m : ℕ) :
superPow (stdSuperPair k ℓ) m ⟶ P.ω.obj { arity := m }

The model transport: iterated strand identifications assembled left-nested through the structure maps.

Equations
Instances For
    noncomputable def RS.stdFromOmega {R : ℕ} (f : EdgeRankParameter R) (P : DelignePackage (SkeinObj f)) {k ℓ : ℕ} (e' : P.ω.obj { arity := 1 } ⟶ stdSuperPair k ℓ) (m : ℕ) :
    P.ω.obj { arity := m } ⟶ superPow (stdSuperPair k ℓ) m

    The reverse model transport.

    Equations
    Instances For
      theorem RS.stdFromOmega_stdToOmega {R : ℕ} (f : EdgeRankParameter R) (P : DelignePackage (SkeinObj f)) {k ℓ : ℕ} (e : stdSuperPair k ℓ ⟶ P.ω.obj { arity := 1 }) (e' : P.ω.obj { arity := 1 } ⟶ stdSuperPair k ℓ) (hee' : CategoryTheory.CategoryStruct.comp e' e = CategoryTheory.CategoryStruct.id (P.ω.obj { arity := 1 })) (m : ℕ) :

      The transports are inverse on the fibre side.

      The transports are inverse on the model side.