HregExplicitKG · section of the QIQT-H book

QIQTH.HregExplicitKG

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HregExplicitKG · entries 445–447 of 1000

Lemma 445 (kgLagr_contDiff).  source ↗

The KG Lagrangian scalar is C^∞.

(φ)∈C∞→(∀(ab:Fin n),(λy↦gab(y))∈C∞)→(kgLagr m φ gi)∈C∞({\varphi})\in C^{\infty} \to (\forall (a b : \mathrm{Fin}\,n), ({\lambda y \mapsto g^{{a}{b}}({y})})\in C^{\infty}) \to ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kglagr}{\mathrm{kgLagr}}\,m\,\varphi\,\mathrm{gi}})\in C^{\infty}

Proof. By contDiff_pd, pd. □\square

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:Fin n),(λy↦gab(y))∈C∞)→(∀(ab:Fin n),(λy↦gab(y))∈C∞)→∀(ab:Fin n),(λy↦T(y) a b)∈C∞({\varphi})\in C^{\infty} \to (\forall (a b : \mathrm{Fin}\,n), ({\lambda y \mapsto g_{{a}{b}}({y})})\in C^{\infty}) \to (\forall (a b : \mathrm{Fin}\,n), ({\lambda y \mapsto g^{{a}{b}}({y})})\in C^{\infty}) \to \forall (a b : \mathrm{Fin}\,n), ({\lambda y \mapsto \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({y})\,a\,b}})\in C^{\infty}

Proof. By contDiff_pd, pd, kgLagr_contDiff, kgLagr. □\square

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:Fin 4),gab(y)=gba(y))→(∀(y:M4)(ab:Fin 4),∑σgaσ(y)⋅gσb(y)=δab)→(φ)∈C∞→(∀(ab:Fin 4),(λy↦gab(y))∈C∞)→(∀(ab:Fin 4),(λy↦gab(y))∈C∞)→∀(f:M4→R),(∀(y:M4)(a′b:Fin 4),a⋅T(y) a′ b=Ra′b(y)+f y⋅ga′b(y))→(∀(x:M4)(ρ:Fin 4),PdiffAt f ρ x)∧Differentiable R λy↦f y+1/2⋅R(y)(\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (a b : \mathrm{Fin}\,4), g^{{a}{b}}({y}) = g^{{b}{a}}({y})) \to (\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (a b : \mathrm{Fin}\,4), \sum_{\sigma} g_{{a}{\sigma}}({y}) \cdot g^{{\sigma}{b}}({y}) = \delta_{ab}) \to ({\varphi})\in C^{\infty} \to (\forall (a b : \mathrm{Fin}\,4), ({\lambda y \mapsto g_{{a}{b}}({y})})\in C^{\infty}) \to (\forall (a b : \mathrm{Fin}\,4), ({\lambda y \mapsto g^{{a}{b}}({y})})\in C^{\infty}) \to \forall (f : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathbb{R}), (\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (a^{\prime} b : \mathrm{Fin}\,4), a \cdot \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({y})\,a^{\prime}\,b} = \href{/browser/qiqth-curvature#d-qiqth-curvature-ricci}{R_{{a^{\prime}}{b}}({y})} + f\,y \cdot g_{{a^{\prime}}{b}}({y})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\rho : \mathrm{Fin}\,4), \href{/browser/qiqth-curvature#d-qiqth-curvature-pdiffat}{\mathrm{PdiffAt}}\,f\,\rho\,x) \wedge \mathrm{Differentiable}\,\mathbb{R}\,\lambda y \mapsto f\,y + 1/2 \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-scalarcurv}{R({y})}

Proof. By scalarCurv_contDiff, PdiffAt_of_contDiff, metric_contraction_trace, kgStress_contDiff. □\square

Used by qiqt_gr_explicit_kg, qiqt_gr_freefield.


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