RECEIPT CLOSED · Phases 1-8 signed · Branch A clean zero + Phase 7 boundary audit + Phase 8 Maxwell completion (A8 / B8) · registered classical-vacuum domain

Shadow Faraday Zero-Out · v0.1 · pre-registered

Do local shadows recover Faraday induction?

A minimal, falsification-first experiment. We define a local, gauge-invariant shadow projection 𝒫shadow and ask whether it is sufficient to close Faraday's law of induction algebraically — without reconstructing the electromagnetic potential Aμ globally. The result lands in one of three pre-registered zones: clean structural zero, named quarantine, or bounded failure. All three ship a receipt. For the AI-safety translation of this same apparatus, see the shadow-method bridge essay.

Phases 1-8 closed · Branch A Phase 4 battery 5/5 Phase 7 boundary audit · A7 / B7 / B7-topology Phase 8 Maxwell completion · A8 / B8 Class A metadata + sitemap pre-registered predicate 𝒫shadow = two-tier coordinate plaquette holonomy gauge invariance audited on registered domain
𝐁 — magnetic field (cool) · 𝒫shadow — local projection · 𝐄 — electric field (warm)
Closing Faraday induction with shadow data alone. A flux surface threaded by magnetic-field arrows is encircled by an electric-field loop. The Faraday integral expression to its right has the shadow projection operator applied to both E and B. The pre-registered predicate evaluates to a large green zero, captioned "structural or named." spanned surface · Σ 𝐁(t) ∂Σ 𝐄 ∂Σ   𝒫shadow ( 𝐄 d𝓁 + d / dt   Σ   𝒫shadow ( 𝐁 d𝐀 PRE-REG SUCCESS PREDICATE → 0 ? STRUCTURAL · OR · NAMED
Equals zero · or names its residual · either outcome ships a receipt.

The Pre-Registered Claim

One algebraic question, three landing zones, all of them publishable.

The Sundog method is allergic to ambiguity, not to negative results. We register the predicate before the algebra runs, then publish whichever of structural zero, named quarantine, or bounded failure falls out. Faraday is the calibration object: too well-understood to fudge, too foundational to ignore.

If 𝒫shadow is the right object, Faraday induction closes locally — no global gauge fix, no field reconstruction at infinity, just the loop and the flux.

This page is a receipt surface: Phase 3 now lands Branch A on the registered classical vacuum domain, and Phase 4 verification / falsification passes 5/5. Phase 5 chapter close is signed, and the page now carries the public metadata, share card, sitemap entry, and internal path.

The Object · I

Antisymmetric, two scalars, gauge-invariant.

All of classical electromagnetism, including Faraday's law, Gauss's law for magnetism, and Lorentz invariance under boosts, compresses into a single 4×4 antisymmetric tensor Fμν = ∂μAν − ∂νAμ and exactly two Lorentz scalars. The shadow apparatus must respect the same symmetries.

Fμν =
0 Ex/c Ey/c Ez/c
−Ex/c 0 −Bz By
−Ey/c Bz 0 −Bx
−Ez/c −By Bx 0
Fμν = ∂μAν − ∂νAμ

Invariant I · scalar density

FμνFμν = 2(B² − E²/c²)

Invariant II · pseudoscalar · CP-odd

Fμνμν = −4 𝐄·𝐁/c

The Apparatus · II

𝒫shadow is the plaquette holonomy on A.

Phase 2 fixes the operator as a two-tier coordinate plaquette holonomy. For a point x, a coordinate plaquette ωμν(x, ε) of edge ε, and the closed boundary loop ∂ω, the finite-stencil operator is the Wilson-loop-style line integral of the potential one-form:

𝒫shadowstencil[A]μν(x, ε)  :=  ∮∂ωμν(x, ε) A  =  ∫ω F  =  ε² · Fμν(x) + O(ε³)

Stokes' theorem turns the line integral of A on the closed loop into the surface integral of F on the plaquette — and F is gauge-invariant by construction. The operator never inspects a globally consistent Aμ: it reads A only on the four edges of one plaquette.

The pre-registered audit predicate is deceptively simple, and load-bearing:

𝒫shadow(A + dλ) ≡ 𝒫shadow(A)

The proof on the registered domain is a single line: ∮∂ω dλ = 0 for any closed loop ∂ω with smooth λ, so the gauge term drops out of the holonomy by Stokes. The audit fails by name outside that domain: five quarantine hooks — regularity, topology, monopole, operator-stencil commutator, motional EMF — are enumerated in the Phase 2 receipt before any Phase 3 algebra runs. The discipline lineage is Isotrophy K_facet v0.3h, whose audit chain landed 20 structural-zero receipts and the named O_617 quarantine on exactly this pre-registration pattern.

Phase 2 receipt: docs/faraday/SHADOW_FARADAY.md ▸ Phase 2: Local Shadow Projection Operator. Phase 2 sign-off decisions are recorded there: coordinate plaquettes, point-limit gate plus finite-stencil locality receipt, no Floquet/twist rescue in Phase 3, and the two-tier operator retained with roles locked.

The Battery · III

Three falsifiers, pre-committed and now run.

Each falsifier is designed to break the claim in a pre-named way. Anything else — any unexpected residual, any silent failure — is the receipt worth writing down. These were registered before Phase 3 algebra ran. Phase 4 passed 5/5: constant B, a source-free plane wave, a nonlocal residual, a monopole quarantine, and gauge invariance.

Non-local probe

Deliberately widen the stencil beyond the locality radius.

observed: residual

Artificial monopole

Inject a source term forbidden by the source-free assumption.

observed: quarantine

Gauge after projection

Apply A → A + dλ after 𝒫shadow has run.

observed: invariant

The Pipeline · IV

Symbol table → public page · six phases · each gated on a signed receipt.

Same discipline as Isotrophy v0.3 and the three-body controller: each phase exits when its receipt is signed off, not when it feels done. Phase 3 — the core zero-out — is the load-bearing algebra; Phase 4 is the support battery; Phase 5 closes the chapter before public dissemination.

1 foundations symbol & map 2 𝒫_shadow operator + gauge audit 3 zero-out ★ core derivation 4 battery 5/5 support battery 5 chapter close receipts + handoff 6 faraday.html public page

The Outcomes · V

Three landing zones. All of them ship.

Pre-registered framing turns every possible Phase 3 result into a public receipt. The discipline is the same one that produced Isotrophy K_facet v0.3h's 20 structural zeros + 1 named quarantine: name the success predicate before the algebra runs; if the result is a partial, the partial is the artifact.

A · clean zero

Structural identity

Shadow projection is sufficient; Faraday induction closes locally with no residual. The strongest claim — and the most demanding receipt.

B · named quarantine

Topological / boundary term

One precisely-named survivor — boundary at infinity, Aharonov–Bohm phase, or a documented global obstruction. Closure is conditional; the failure is articulate.

C · bounded failure

Reconstruction survives

Shadow projection is insufficient at order X. The bound is publishable, the prior is updated, the scope is corrected.

The Boundary · VI · Phase 7

Three steps off the clean domain — each named before the algebra ran.

Phase 7 does not broaden Branch A; it audits the first boundary around it. Three nearby cases were registered with their expected landings before any computation, then derived by hand and mirrored by a seconds-scale battery (npm run faraday:phase7). All three landed where pre-registered — no surprise residual in any clean, contractible computation.

A7 · clean control

Electric sources are invisible

Add a real current (Jμ ≠ 0) but keep dF = 0: the Faraday residual stays an exact zero. Electric sources live in the inhomogeneous law d⋆F = J, never in dF — closure is source-tolerant in the narrow Bianchi sense only, not a full-Maxwell claim.

B7 · magnetic source

A named magnetic flux

Insert a registered magnetic charge (dF = Km ≠ 0): the survivor is exactly the magnetic flux Qm through the audited volume — named and accounted, not a clean-domain failure.

B7 · topology ★

The Aharonov–Bohm survivor

Encircle a solenoid where F = 0: the local field reads nothing, yet the loop holonomy ∮A = Φ survives — the enclosed flux, an exact topological invariant (H1).

The two tiers of 𝒫shadow diverge by exactly Φ: the point-tier field F = 0 is blind, but the loop-tier holonomy ∮A = Φ is decisive. A shadow that cannot reconstruct the state can still be sufficient for the decision — here exactly, set by topology rather than approximation.

Phase 7 receipt: docs/faraday/FARADAY_PHASE7_BOUNDARY.md · branches A7-clean-control / B7-magnetic-source / B7-topology · support battery npm run faraday:phase7. Classical only; single-valued λ keeps Φ exactly gauge-invariant. For the cross-substrate reading — the first exact shadow-decides-without-reconstructing separation in the portfolio, bounded to topological scale — see the public body-resistance vocabulary.

The Completion · VII · Phase 8

The other half of Maxwell — and why Aharonov–Bohm was the only sharp witness.

Faraday is the homogeneous half (dF = 0, an identity). Phase 8 turns to the inhomogeneous half d⋆F = J — the sourced, metric-bearing side — through a dual shadow 𝒫shadowdual = ∮⋆F. Three registered cases, hand-derived and mirrored by a seconds-scale battery (npm run faraday:phase8), landed exactly where pre-registered.

A8 · Gauss

The dual of the monopole

The dual shadow recovers Gauss's law: ∮⋆F = Qenc. Electric charge lives in d⋆F = J exactly where magnetic charge broke dF = 0 in Phase 7 — the Hodge star is the swap, and the place the metric finally enters.

A8 · Ampère–Maxwell

Displacement current closes the loop

With a time-varying field the dual shadow returns ∮B·d𝓁 = Ienc + d/dt ΦE — conduction plus the distinctively-Maxwell displacement current. The battery matches to thirteen digits.

B8 · Hodge split ★

No new sharp separation

On a topological domain the field splits into a sourced piece (determined by its charge) and a harmonic piece (= the Phase 7 Aharonov–Bohm flux). The dual shadow reads the charge; the loop shadow reads the flux — orthogonal sectors.

The whole classical field is (sources, boundary, harmonic periods). All of the shadow's exact regime-2 content lives in the harmonic periods — which is why Aharonov–Bohm (Phase 7) was the unique sharp witness. Maxwell adds no new one.

Phase 8 receipt: docs/faraday/FARADAY_PHASE8_BOUNDARY.md · branches A8-dual-closure / B8-harmonic-survivor · support battery npm run faraday:phase8. The dual-shadow closure recovers the integral form of the inhomogeneous law — it is not a re-derivation of Maxwell. Static / given-source domain; free radiation, retarded dynamics, and curved spacetime are named deferrals.

Where This Sits

Faraday is the calibration receipt; Generality is the stress test.

Shadow Faraday is the clean-room version of the Sundog pattern: define a local shadow, pre-register the branch table, let the algebra land, and keep the boundary named. The result closes because classical electromagnetism is already understood; the contribution is the audit shape, not a new law of physics.

The High-Stakes Generality page asks what happens when the same discipline is carried into domains where the answer is not known in advance or the result is bounded-null: Navier-Stokes C1, Riemann, Yang-Mills, P-vs-NP, ARC-AGI, and Three-Body. Read Faraday as the method receipt, then Generality as the harder transfer matrix.

Claim Boundary

Not a universal result.

The experiment closed Branch A on the registered classical-vacuum domain. Phase 7 audited the first boundary off it — electric sources, magnetic sources, and the Aharonov–Bohm topology — each landing as a named survivor, not a broadened claim. Distributional fields, curved spacetime, quantum EM, plasma, and moving surfaces remain named limitations, not silent claims.

Not a derivation of Maxwell.

Phase 8 closed the sourced side too — the dual shadow ∮⋆F = Qenc recovers Gauss and Ampère–Maxwell — but closure recovers the integral form of an already-given law. It is not a re-derivation of the Maxwell system from shadow primitives.

Not a claim about AI.

For the AI-safety translation of the same apparatus, see the dedicated bridge essay at /safety-method, marked SKETCH and load-bearing on this Branch A receipt as its worked example.

Inspection Trail