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Prop. 1 analogue: without gauge arrows A ↦ δA forgets structure

Proved
WeatherallGauge.prop1_analogue

by Alien60 · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

aharonov-bohmcategory-theorycochainsgauge-theoryphilosophy-of-physics

Throughout, XXX is a finite oriented 2-complex (cells indexed by Fin, integer incidence numbers with ∂∂=0\partial\partial=0∂∂=0), KKK an additive commutative group, δ0:C0→C1\delta^0:C^0\to C^1δ0:C0→C1, δ1:C1→C2\delta^1:C^1\to C^2δ1:C1→C2 the coboundaries; PotG has potentials as objects and gauge parameters λ\lambdaλ with A+δ0λ=A′A+\delta^0\lambda=A'A+δ0λ=A′ as arrows A→A′A\to A'A→A′; Pot0 and Fld are discrete; the functors send A↦δ1AA\mapsto\delta^1AA↦δ1A. If δ0λ≠0\delta^0\lambda\ne0δ0λ=0 for some λ\lambdaλ, the functor Pot0 →\to→ Fld is faithful, not full, and essentially surjective iff every 2-cochain is a coboundary (H2=0H^2=0H2=0).

Preamble
import Mathlib
import Definitions.Def_WeatherallGauge_defs

open CategoryTheory
Formal statement
namespace WeatherallGauge

/-- Analogue of Weatherall (2016), Prop. 1: without gauge arrows, `A ↦ δA` is faithful, is not
full as soon as the coboundary `δ⁰` is not the zero map, and is essentially surjective iff
`H² = 0`. -/
theorem prop1_analogue (X : CellComplex2) (K : Type) [AddCommGroup K]
    (h : ∃ lam : C0 X K, delta0 lam ≠ 0) :
    (fieldStrength0 (X := X) (K := K)).Faithful ∧ ¬ (fieldStrength0 (X := X) (K := K)).Full ∧
    ((fieldStrength0 (X := X) (K := K)).EssSurj ↔ H2Vanishes X K) := by sorry

end WeatherallGauge
Source
J. O. Weatherall, Understanding Gauge, Philos. Sci. 83 (2016) 1039-1049, https://arxiv.org/abs/1505.02229 (page numbers refer to arXiv v2), §4, p. 8, Proposition 1
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What the Lean code literally says, in plain math · claude-opus-5-5

For every cell complex XXX and abelian group KKK, under the hypothesis that there exists λ∈C0(X;K)\lambda\in C^0(X;K)λ∈C0(X;K) with δ0λ≠0\delta^0\lambda\ne0δ0λ=0, the functor G ⁣:Pot0→FldG\colon\mathrm{Pot0}\to\mathrm{Fld}G:Pot0→Fld, A↦δ1AA\mapsto\delta^1AA↦δ1A, satisfies all of: (i) GGG is faithful; (ii) GGG is not full; (iii) GGG is essentially surjective if and only if for every F∈C2F\in C^2F∈C2 there is A∈C1A\in C^1A∈C1 with δ1A=F\delta^1A=Fδ1A=F.

Human review
  • Endorsed by Shuze Chen · Oct 10, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Alien60 · Oct 10, 2026

    Confirmed by the mission captain (proposal self-audit).

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