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DefinitionDefinition: Literature-sourcedProof: AI-adaptedPipeline-generatedverified 2026-10-15 (gpt-6-luna, gpt-6.1-sol, and delegated Codex review/repair agents; see completed run evidence)
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Free transverse-photon energy multiplier

Definition

Assume Countable Choice The Axiom of Countable Choice (ACω). Use the transverse space HT=Ran⁡MPT of Positive transverse photon one-particle space, with PT(k)=I3−nnT for k≠0 and any assigned value at the null point k=0. In the QFT length convention, assign k units m−1 and define the nonnegative measurable multiplier ω(k):=∣k∣. Its maximal multiplication operator on HT is (Mωf)(k):=ω(k)f(k),D(Mω):={f∈HT:ωf∈L2(R3,d3k;C3)}. Because ω is a scalar multiplier, k⋅f(k)=0 a.e. implies k⋅(Mωf)(k)=0 a.e.; thus the displayed multiplication maps its stated domain into HT. The value ω(0)=0 is immaterial to the L2 operator. For ℏ,c>0, the corresponding one-particle energy convention is E1:=ℏcMω, in joules.

Remarks

The QFT-MG01 transverse-space draft is present and its exact projection-space definition was inspected, and its page manifest lists the draft supplier items. This local multiplier is conditional on that mathematical supplier. No photon polarization frame, interacting dynamics, or empirical photon-energy claim is part of this definition.

Facts & Assumptions

Given: The transverse-space interface, ℏ>0 in J s, c>0 in m s−1, and k in m−1.

[A1]

The stated units and positivity of ℏ,c are model conventions in this definition.

[A2]

Assume Countable Choice, as required by the transverse-space supplier. The Axiom of Countable Choice (ACω)

[F1]

Positive transverse photon one-particle space defines HT=Ran⁡MPT as the vector-valued L2 subspace with k⋅f(k)=0 a.e.; the draft carrier exists and is listed in the QFT-MG01 manifest. This mathematical use retains its supplier hypotheses and does not itself confer independent acceptance.

[F2]

Cauchy–Schwarz: ∣⟨u,v⟩∣≤∥u∥∥v∥, with equality exactly for linearly dependent vectors: ∣⟨u,v⟩∣≤∥u∥∥v∥ in a real or complex inner-product space.

Proof

1.1A2F1givenalgebra

The norm map k↦∣k∣ is measurable and nonnegative. If f∈D(Mω), then ωf is square-integrable by the stated domain and k⋅(ωf)=ω(k⋅f)=0 a.e.; [F1] therefore places Mωf in HT. Thus the maximal multiplication operator is well-defined on its stated domain.

2.1A1A2F2step 1.1algebra∎

Since [ω]=m−1 and [ℏc]=J m, E1=ℏcMω has energy units. For f∈D(Mω), [F2] gives ∣⟨f,Mωf⟩2∣≤∥f∥2∥Mωf∥2<∞; the integral representation is ∫∣k∣∣f(k)∣2d3k≥0 because ω≥0. Hence E1 is nonnegative on its domain.

Depends on

Dependency tree · 2 levels

Sources