HregExplicitKG · section of the QIQT-H book
QIQTH.HregExplicitKG
← all sections · ← GaussianMode · KGStressConservation →
HregExplicitKG · entries 445–447 of 1000
Lemma 445 (kgLagr_contDiff). source ↗
The KG Lagrangian scalar is C^∞.
(φ)∈C∞→(∀(ab:Finn),(λy↦gab(y))∈C∞)→(kgLagrmφgi)∈C∞
Proof. By contDiff_pd, pd. □
Used by kgStress_contDiff.
Lemma 446 (kgStress_contDiff). source ↗
The KG stress tensor component y ↦ kgStress m φ g gi y a b is C^∞.
(φ)∈C∞→(∀(ab:Finn),(λy↦gab(y))∈C∞)→(∀(ab:Finn),(λy↦gab(y))∈C∞)→∀(ab:Finn),(λy↦T(y)ab)∈C∞
Proof. By contDiff_pd, pd, kgLagr_contDiff, kgLagr. □
Used by hreg_kg.
Lemma 447 (hreg_kg). source ↗
The hreg input, DISCHARGED for the explicit free Klein–Gordon field (Tier A4). For any focusing scalar f satisfying a·kgStress = Ric + f·g, the gi-trace fixes f = (a·tr(kgStress) − R)/4 (using ∑ gi·g = 4), which is C^∞; hence f is differentiable everywhere and f + ½R is differentiable.
(∀(y:M4)(ab:Fin4),gab(y)=gba(y))→(∀(y:M4)(ab:Fin4),σ∑gaσ(y)⋅gσb(y)=δab)→(φ)∈C∞→(∀(ab:Fin4),(λy↦gab(y))∈C∞)→(∀(ab:Fin4),(λy↦gab(y))∈C∞)→∀(f:M4→R),(∀(y:M4)(a′b:Fin4),a⋅T(y)a′b=Ra′b(y)+fy⋅ga′b(y))→(∀(x:M4)(ρ:Fin4),PdiffAtfρx)∧DifferentiableRλy↦fy+1/2⋅R(y)
Proof. By scalarCurv_contDiff, PdiffAt_of_contDiff, metric_contraction_trace, kgStress_contDiff. □
Used by qiqt_gr_explicit_kg, qiqt_gr_freefield.
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