QiqtGrFreeField · section of the QIQT-H book

QIQTH.QiqtGrFreeField

← all sections · ← QiqtGrExplicitKG · QiqtGrGaussian →

QiqtGrFreeField · entries 549–555 of 1000

Lemma 549 (BL_kgStress_null). source ↗

Stage 0 (T3-3): the KG null-stress simplification. On the null cone BL(g x) v = 0, the Klein–Gordon stress tensor’s null component collapses to the squared directional derivative BL(kgStress) v = (∑ₐ vₐ ∂ₐφ)² — because the trace term −½ g_{ab} L contracts to −½·(BL(g x)v)·L = 0. This is the classical null-energy T_kk = (v^a ∂_a φ)² that the localization map (hTkk) identifies with the one-particle rapidity-momentum integral. Axiom-free, reusable.

\href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v}) = {(\sum_{a} v\,a \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-pd}{\partial_{{a}}({\varphi})({x})})}^{2}

Proof. By kgLagr. $\square$

Used by qiqt_gr_freefield_nullEnergy.

Lemma 550 (freeField_kd_conclusion). source ↗

The free-field flux equation kd x v = (2π/ℏ)·BL(T x)v, per null generator. The ∀-wrap of freeField_component_hFlux: given, for each null horizon generator (x,v), a smooth wedge mode f_{x,v} (with the standard integrability/measurability/bound data) together with - hbridge : the abstract coefficient kd x v IS the modular energy of the localized mode, and - hTkk : the localization identification of BL(T x)v with the mode’s rapidity stress flux, derivative uniqueness against the axiom-free freeField_oneParticle_hFlux yields the flux equation. This is the exact input qiqt_gr_from_flux_complete (hence qiqt_bekenstein_gives_gr) consumes. …

(\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{Integrable}\,(f\,x\,v)\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), ({f\,x\,v})'({\theta})={f^{\prime}\,x\,v\,\theta}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{AEStronglyMeasurable}\,(f^{\prime}\,x\,v)\,\mathrm{vol}) \to \forall (B : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), \|f^{\prime}\,x\,v\,\theta\| \le B\,x\,v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to 2 \cdot \pi / \hbar \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({T\,x})({v},{v})} = (-(2 \cdot \pi \cdot \int (\theta : \mathbb{R}), (\mathrm{starRingEnd}\,\mathbb{C})\,(f\,x\,v\,\theta) \cdot f^{\prime}\,x\,v\,\theta)).\mathrm{im}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\lambda t \mapsto \langle {\mathrm{toLp}\,(f\,x\,v)\,\cdots },{(\href{/browser/qiqth-standardsubspacemodularflow#d-qiqth-standardsubspacemodular-modunitary}{\Delta}\,(\href{/browser/qiqth-fock-boostkms#d-qiqth-fock-boostkms-nicewedgestandardsubspace}{\mathcal{K}}\,(\mathrm{mw}\,x\,v)\,\cdots \,\cdots )\,t)\,(\mathrm{toLp}\,(f\,x\,v)\,\cdots )}\rangle})'({0})={i \cdot (\dot{K}({x},{v}))}) \to \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \dot{K}({x},{v}) = 2 \cdot \pi / \hbar \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({T\,x})({v},{v})}

Proof. By freeField_component_hFlux. $\square$

Used by qiqt_gr_freefield.

Theorem 551 (qiqt_gr_freefield). source ↗

THE FREE-FIELD QIQT→GR CAPSTONE. Einstein’s equations for the explicit free Klein–Gordon field, with the wedge-KMS modular flux supplied entirely by the axiom-free +2π one-particle Bisognano–Wichmann machinery — NOT a labelled WedgeKMSFlux_complete bundle. Identical to qiqt_gr_explicit_kg (geometry hC/hric_symm/hreg, matter conserv, and hT_symm all discharged internally for kgStress), but the modular input is the per-null-generator localization datum (mw, f, f', …, hTkk, hbridge) feeding freeField_kd_conclusion. …

(\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), 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 (\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 (\varphi : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathbb{R}) (m \eta \hbar a : \mathbb{R}), \hbar \ne 0 \to \eta \ne 0 \to a = 2 \cdot \pi / (\hbar \cdot \eta) \to ({\varphi})\in C^{\infty} \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}), \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-boxfield}{(\Box {\varphi})({x})} = {m}^{2} \cdot \varphi\,x) \to \forall (P \mathrm{Pinv} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} P_{{i}{k}}({x}) \cdot (P^{-1})_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} (P^{-1})_{{i}{k}}({x}) \cdot P_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), g_{{i}{j}}({x}) = \sum_{k} \sum_{l} P_{{k}{i}}({x}) \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-gm}{\eta_{{k}{l}}} \cdot P_{{l}{j}}({x})) \to \forall (\mathrm{Sf} \mathrm{KE} A : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{R}) (\mathrm{sd} \mathrm{kd} \mathrm{ad} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{Sf}\,x\,v})'({0})={\dot{S}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{KE}\,x\,v})'({0})={\dot{K}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({A\,x\,v})'({0})={\dot{A}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \text{for }t\text{ near }0,\; \mathrm{Sf}\,x\,v\,t \le \eta \cdot A({x},{v},{t})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{Sf}\,x\,v\,0 = \eta \cdot A({x},{v},{0})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \forall (t : \mathbb{R}), 0 \le \mathrm{KE}({x},{v},{t}) - \mathrm{Sf}\,x\,v\,t) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{KE}({x},{v},{0}) - \mathrm{Sf}\,x\,v\,0 = 0) \to \forall (\mathrm{mw} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}) (\mathrm{hmw} : \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), 0 < \mathrm{mw}\,x\,v) (\mathrm{ff} \mathrm{ff}^{\prime} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{C}) (\mathrm{hf2} : \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{MemLp}\,(\mathrm{ff}\,x\,v)\,2\,\mathrm{vol}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{Integrable}\,(\mathrm{ff}\,x\,v)\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), ({\mathrm{ff}\,x\,v})'({\theta})={\mathrm{ff}^{\prime}\,x\,v\,\theta}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{AEStronglyMeasurable}\,(\mathrm{ff}^{\prime}\,x\,v)\,\mathrm{vol}) \to \forall (\mathrm{Bd} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), \|\mathrm{ff}^{\prime}\,x\,v\,\theta\| \le \mathrm{Bd}\,x\,v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to 2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v}) = (-(2 \cdot \pi \cdot \int (\theta : \mathbb{R}), (\mathrm{starRingEnd}\,\mathbb{C})\,(\mathrm{ff}\,x\,v\,\theta) \cdot \mathrm{ff}^{\prime}\,x\,v\,\theta)).\mathrm{im}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\lambda t \mapsto \langle {\mathrm{toLp}\,(\mathrm{ff}\,x\,v)\,\cdots },{(\href{/browser/qiqth-standardsubspacemodularflow#d-qiqth-standardsubspacemodular-modunitary}{\Delta}\,(\href{/browser/qiqth-fock-boostkms#d-qiqth-fock-boostkms-nicewedgestandardsubspace}{\mathcal{K}}\,(\mathrm{mw}\,x\,v)\,\cdots \,\cdots )\,t)\,(\mathrm{toLp}\,(\mathrm{ff}\,x\,v)\,\cdots )}\rangle})'({0})={i \cdot (\dot{K}({x},{v}))}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \dot{A}({x},{v}) = ({\lambda i j \mapsto \href{/browser/qiqth-curvature#d-qiqth-curvature-ricci}{R_{{i}{j}}({x})}})({v},{v})) \to \exists \Lambda, \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu \nu : \mathrm{Fin}\,4), a \cdot \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})\,\mu\,\nu} = \href{/browser/qiqth-curvature#d-qiqth-curvature-einsteintensor}{G_{{\mu}{\nu}}({x})} + \Lambda \cdot g_{{\mu}{\nu}}({x})

Proof. By pd, PdiffAt, scalarCurv, hreg_kg, kgLagr, kg_conserv_of_contDiff, freeField_kd_conclusion, qiqt_gr_from_flux_complete. $\square$

Used by qiqt_gr_freefield_localized.

Theorem 552 (qiqt_gr_freefield_localized). source ↗

Stage 1 (T3-3): hbridge discharged. The free-field QIQT→GR capstone with the heat coefficient FIXED to the boost flux kd x v := (2π/ℏ)·BL(kgStress) v and the modular-localization hypothesis hbridge DERIVED internally from freeField_oneParticle_hFlux (the axiom-free +2π one-particle Bisognano–Wichmann machinery) given hTkk. The thermodynamic premise hK now reads HasDerivAt (KE x v) ((2π/ℏ)·T_kk) 0 — the genuine Clausius statement that the heat-functional rate IS the boost-energy flux (correctly kept labelled). Of the Gap-2 localization map only hTkk (Stage 3) and the focusing identity hFocus (Stage 2) survive as inputs. Axiom-free.

(\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), 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 (\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 (\varphi : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathbb{R}) (m \eta \hbar a : \mathbb{R}), \hbar \ne 0 \to \eta \ne 0 \to a = 2 \cdot \pi / (\hbar \cdot \eta) \to ({\varphi})\in C^{\infty} \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}), \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-boxfield}{(\Box {\varphi})({x})} = {m}^{2} \cdot \varphi\,x) \to \forall (P \mathrm{Pinv} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} P_{{i}{k}}({x}) \cdot (P^{-1})_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} (P^{-1})_{{i}{k}}({x}) \cdot P_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), g_{{i}{j}}({x}) = \sum_{k} \sum_{l} P_{{k}{i}}({x}) \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-gm}{\eta_{{k}{l}}} \cdot P_{{l}{j}}({x})) \to \forall (\mathrm{Sf} \mathrm{KE} A : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{R}) (\mathrm{sd} \mathrm{ad} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{Sf}\,x\,v})'({0})={\dot{S}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{KE}\,x\,v})'({0})={2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({A\,x\,v})'({0})={\dot{A}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \text{for }t\text{ near }0,\; \mathrm{Sf}\,x\,v\,t \le \eta \cdot A({x},{v},{t})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{Sf}\,x\,v\,0 = \eta \cdot A({x},{v},{0})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \forall (t : \mathbb{R}), 0 \le \mathrm{KE}({x},{v},{t}) - \mathrm{Sf}\,x\,v\,t) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{KE}({x},{v},{0}) - \mathrm{Sf}\,x\,v\,0 = 0) \to \forall (\mathrm{mw} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), 0 < \mathrm{mw}\,x\,v) \to \forall (\mathrm{ff} \mathrm{ff}^{\prime} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{C}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{MemLp}\,(\mathrm{ff}\,x\,v)\,2\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{Integrable}\,(\mathrm{ff}\,x\,v)\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), ({\mathrm{ff}\,x\,v})'({\theta})={\mathrm{ff}^{\prime}\,x\,v\,\theta}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{AEStronglyMeasurable}\,(\mathrm{ff}^{\prime}\,x\,v)\,\mathrm{vol}) \to \forall (\mathrm{Bd} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), \|\mathrm{ff}^{\prime}\,x\,v\,\theta\| \le \mathrm{Bd}\,x\,v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to 2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v}) = (-(2 \cdot \pi \cdot \int (\theta : \mathbb{R}), (\mathrm{starRingEnd}\,\mathbb{C})\,(\mathrm{ff}\,x\,v\,\theta) \cdot \mathrm{ff}^{\prime}\,x\,v\,\theta)).\mathrm{im}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \dot{A}({x},{v}) = ({\lambda i j \mapsto \href{/browser/qiqth-curvature#d-qiqth-curvature-ricci}{R_{{i}{j}}({x})}})({v},{v})) \to \exists \Lambda, \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu \nu : \mathrm{Fin}\,4), a \cdot \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})\,\mu\,\nu} = \href{/browser/qiqth-curvature#d-qiqth-curvature-einsteintensor}{G_{{\mu}{\nu}}({x})} + \Lambda \cdot g_{{\mu}{\nu}}({x})

Proof. By freeField_oneParticle_hFlux, qiqt_gr_freefield. $\square$

Used by qiqt_gr_freefield_localized'.

Theorem 553 (qiqt_gr_freefield_localized'). source ↗

Stage 2 (T3-3): hFocus discharged via Raychaudhuri. The localized free-field capstone with the focusing identity hFocus (ad = R_kk) no longer assumed but DERIVED from the machine-checked Raychaudhuri equation (hFocus_of_raychaudhuri): per null generator (x,v) we supply a smooth geodesic congruence W x v through (x,v) (hWx : W x v x = v), at equilibrium (hWequil, the shear–expansion quadratic vanishes — Jacobson’s stationary/bifurcation horizon), with the area-vs-expansion identification hWarea. The Raychaudhuri focusing law ad = BL(Ric) v is then proved (no Einstein presupposed); christoffel smoothness is itself discharged (christoffel_contDiff). …

(\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), 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 (\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 (\varphi : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathbb{R}) (m \eta \hbar a : \mathbb{R}), \hbar \ne 0 \to \eta \ne 0 \to a = 2 \cdot \pi / (\hbar \cdot \eta) \to ({\varphi})\in C^{\infty} \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}), \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-boxfield}{(\Box {\varphi})({x})} = {m}^{2} \cdot \varphi\,x) \to \forall (P \mathrm{Pinv} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} P_{{i}{k}}({x}) \cdot (P^{-1})_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} (P^{-1})_{{i}{k}}({x}) \cdot P_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), g_{{i}{j}}({x}) = \sum_{k} \sum_{l} P_{{k}{i}}({x}) \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-gm}{\eta_{{k}{l}}} \cdot P_{{l}{j}}({x})) \to \forall (\mathrm{Sf} \mathrm{KE} A : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{R}) (\mathrm{sd} \mathrm{ad} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{Sf}\,x\,v})'({0})={\dot{S}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{KE}\,x\,v})'({0})={2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({A\,x\,v})'({0})={\dot{A}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \text{for }t\text{ near }0,\; \mathrm{Sf}\,x\,v\,t \le \eta \cdot A({x},{v},{t})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{Sf}\,x\,v\,0 = \eta \cdot A({x},{v},{0})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \forall (t : \mathbb{R}), 0 \le \mathrm{KE}({x},{v},{t}) - \mathrm{Sf}\,x\,v\,t) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{KE}({x},{v},{0}) - \mathrm{Sf}\,x\,v\,0 = 0) \to \forall (\mathrm{mw} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), 0 < \mathrm{mw}\,x\,v) \to \forall (\mathrm{ff} \mathrm{ff}^{\prime} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{C}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{MemLp}\,(\mathrm{ff}\,x\,v)\,2\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{Integrable}\,(\mathrm{ff}\,x\,v)\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), ({\mathrm{ff}\,x\,v})'({\theta})={\mathrm{ff}^{\prime}\,x\,v\,\theta}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{AEStronglyMeasurable}\,(\mathrm{ff}^{\prime}\,x\,v)\,\mathrm{vol}) \to \forall (\mathrm{Bd} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), \|\mathrm{ff}^{\prime}\,x\,v\,\theta\| \le \mathrm{Bd}\,x\,v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to 2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v}) = (-(2 \cdot \pi \cdot \int (\theta : \mathbb{R}), (\mathrm{starRingEnd}\,\mathbb{C})\,(\mathrm{ff}\,x\,v\,\theta) \cdot \mathrm{ff}^{\prime}\,x\,v\,\theta)).\mathrm{im}) \to \forall (W : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to W\,x\,v\,x = v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\mu : \mathrm{Fin}\,4), ({\lambda y \mapsto W\,x\,v\,y\,\mu})\in C^{\infty}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu : \mathrm{Fin}\,4), \sum_{\nu} W\,x\,v\,y\,\nu \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\nu}}{}^{{\mu}}({y})} = 0) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \sum_{\mu} \sum_{\nu} \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\mu}}{}^{{\nu}}({x})} \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\nu}}{}^{{\mu}}({x})} = 0) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \dot{A}({x},{v}) = -\sum_{\nu} W\,x\,v\,x\,\nu \cdot \partial_{{\nu}}({\lambda y \mapsto \href{/browser/qiqth-raychaudhuri#d-qiqth-curvature-expansion}{\theta({y})}})({x})) \to \exists \Lambda, \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu \nu : \mathrm{Fin}\,4), a \cdot \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})\,\mu\,\nu} = \href{/browser/qiqth-curvature#d-qiqth-curvature-einsteintensor}{G_{{\mu}{\nu}}({x})} + \Lambda \cdot g_{{\mu}{\nu}}({x})

Proof. By christoffel_contDiff, ricci, qiqt_gr_freefield_localized, hFocus_of_raychaudhuri. $\square$

Used by qiqt_gr_freefield_nullEnergy.

Theorem 554 (qiqt_gr_freefield_nullEnergy). source ↗

Stage 3 (T3-3): hTkk in transparent form — the single irreducible localization input. Identical to qiqt_gr_freefield_localized', but the one surviving Gap-2 input hTkk is stated in its physically transparent form via the Stage-0 null-stress identity BL(kgStress) v = (∑ₐ vₐ ∂ₐφ)²:

2π/ℏ · (∑ₐ vₐ ∂ₐφ(x))² = (−2π ∫ conj(ff x v)·ff' x v).im. …

(\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), 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 (\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 (\varphi : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathbb{R}) (m \eta \hbar a : \mathbb{R}), \hbar \ne 0 \to \eta \ne 0 \to a = 2 \cdot \pi / (\hbar \cdot \eta) \to ({\varphi})\in C^{\infty} \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}), \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-boxfield}{(\Box {\varphi})({x})} = {m}^{2} \cdot \varphi\,x) \to \forall (P \mathrm{Pinv} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} P_{{i}{k}}({x}) \cdot (P^{-1})_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} (P^{-1})_{{i}{k}}({x}) \cdot P_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), g_{{i}{j}}({x}) = \sum_{k} \sum_{l} P_{{k}{i}}({x}) \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-gm}{\eta_{{k}{l}}} \cdot P_{{l}{j}}({x})) \to \forall (\mathrm{Sf} \mathrm{KE} A : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{R}) (\mathrm{sd} \mathrm{ad} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{Sf}\,x\,v})'({0})={\dot{S}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{KE}\,x\,v})'({0})={2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({A\,x\,v})'({0})={\dot{A}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \text{for }t\text{ near }0,\; \mathrm{Sf}\,x\,v\,t \le \eta \cdot A({x},{v},{t})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{Sf}\,x\,v\,0 = \eta \cdot A({x},{v},{0})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \forall (t : \mathbb{R}), 0 \le \mathrm{KE}({x},{v},{t}) - \mathrm{Sf}\,x\,v\,t) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{KE}({x},{v},{0}) - \mathrm{Sf}\,x\,v\,0 = 0) \to \forall (\mathrm{mw} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), 0 < \mathrm{mw}\,x\,v) \to \forall (\mathrm{ff} \mathrm{ff}^{\prime} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{C}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{MemLp}\,(\mathrm{ff}\,x\,v)\,2\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{Integrable}\,(\mathrm{ff}\,x\,v)\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), ({\mathrm{ff}\,x\,v})'({\theta})={\mathrm{ff}^{\prime}\,x\,v\,\theta}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{AEStronglyMeasurable}\,(\mathrm{ff}^{\prime}\,x\,v)\,\mathrm{vol}) \to \forall (\mathrm{Bd} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), \|\mathrm{ff}^{\prime}\,x\,v\,\theta\| \le \mathrm{Bd}\,x\,v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to 2 \cdot \pi / \hbar \cdot {(\sum_{b} v\,b \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-pd}{\partial_{{b}}({\varphi})({x})})}^{2} = (-(2 \cdot \pi \cdot \int (\theta : \mathbb{R}), (\mathrm{starRingEnd}\,\mathbb{C})\,(\mathrm{ff}\,x\,v\,\theta) \cdot \mathrm{ff}^{\prime}\,x\,v\,\theta)).\mathrm{im}) \to \forall (W : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to W\,x\,v\,x = v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\mu : \mathrm{Fin}\,4), ({\lambda y \mapsto W\,x\,v\,y\,\mu})\in C^{\infty}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu : \mathrm{Fin}\,4), \sum_{\nu} W\,x\,v\,y\,\nu \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\nu}}{}^{{\mu}}({y})} = 0) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \sum_{\mu} \sum_{\nu} \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\mu}}{}^{{\nu}}({x})} \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\nu}}{}^{{\mu}}({x})} = 0) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \dot{A}({x},{v}) = -\sum_{\nu} W\,x\,v\,x\,\nu \cdot \partial_{{\nu}}({\lambda y \mapsto \href{/browser/qiqth-raychaudhuri#d-qiqth-curvature-expansion}{\theta({y})}})({x})) \to \exists \Lambda, \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu \nu : \mathrm{Fin}\,4), a \cdot \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})\,\mu\,\nu} = \href{/browser/qiqth-curvature#d-qiqth-curvature-einsteintensor}{G_{{\mu}{\nu}}({x})} + \Lambda \cdot g_{{\mu}{\nu}}({x})

Proof. By BL_kgStress_null, qiqt_gr_freefield_localized'. $\square$

Used by qiqt_gr_freefield_geom, qiqt_gr_freefield_gaussian.

Theorem 555 (qiqt_gr_freefield_geom). source ↗

Stage 2′ (T3-3, option b): hWarea discharged — ad defined geometrically. Identical to qiqt_gr_freefield_nullEnergy, but the area first-variation rate ad is no longer an abstract parameter paired with the labelled identity hWarea; it is defined as the congruence-expansion derivative ad x v := −∑ᵥ Wˣᵛ ∂ᵥ θ[Wˣᵛ], so hWarea becomes rfl. hA (the area functional’s rate) now reads in that explicit geometric form. …

(\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), 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 (\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 (\varphi : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathbb{R}) (m \eta \hbar a : \mathbb{R}), \hbar \ne 0 \to \eta \ne 0 \to a = 2 \cdot \pi / (\hbar \cdot \eta) \to ({\varphi})\in C^{\infty} \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}), \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-boxfield}{(\Box {\varphi})({x})} = {m}^{2} \cdot \varphi\,x) \to \forall (P \mathrm{Pinv} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} P_{{i}{k}}({x}) \cdot (P^{-1})_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), \sum_{k} (P^{-1})_{{i}{k}}({x}) \cdot P_{{k}{j}}({x}) = \delta_{ij}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (i j : \mathrm{Fin}\,4), g_{{i}{j}}({x}) = \sum_{k} \sum_{l} P_{{k}{i}}({x}) \cdot \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-gm}{\eta_{{k}{l}}} \cdot P_{{l}{j}}({x})) \to \forall (\mathrm{Sf} \mathrm{KE} A : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{R}) (\mathrm{sd} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}) (W : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to \mathrm{Fin}\,4 \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to W\,x\,v\,x = v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\mu : \mathrm{Fin}\,4), ({\lambda y \mapsto W\,x\,v\,y\,\mu})\in C^{\infty}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu : \mathrm{Fin}\,4), \sum_{\nu} W\,x\,v\,y\,\nu \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\nu}}{}^{{\mu}}({y})} = 0) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \sum_{\mu} \sum_{\nu} \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\mu}}{}^{{\nu}}({x})} \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-covderivvec}{(\nabla {W\,x\,v})_{{\nu}}{}^{{\mu}}({x})} = 0) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{Sf}\,x\,v})'({0})={\dot{S}({x},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({\mathrm{KE}\,x\,v})'({0})={2 \cdot \pi / \hbar \cdot ({\href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})}})({v},{v})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to ({A\,x\,v})'({0})={-\sum_{\nu} W\,x\,v\,x\,\nu \cdot \partial_{{\nu}}({\lambda y \mapsto \href{/browser/qiqth-raychaudhuri#d-qiqth-curvature-expansion}{\theta({y})}})({x})}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \text{for }t\text{ near }0,\; \mathrm{Sf}\,x\,v\,t \le \eta \cdot A({x},{v},{t})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{Sf}\,x\,v\,0 = \eta \cdot A({x},{v},{0})) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \forall (t : \mathbb{R}), 0 \le \mathrm{KE}({x},{v},{t}) - \mathrm{Sf}\,x\,v\,t) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to \mathrm{KE}({x},{v},{0}) - \mathrm{Sf}\,x\,v\,0 = 0) \to \forall (\mathrm{mw} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), 0 < \mathrm{mw}\,x\,v) \to \forall (\mathrm{ff} \mathrm{ff}^{\prime} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R} \to \mathbb{C}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{MemLp}\,(\mathrm{ff}\,x\,v)\,2\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{Integrable}\,(\mathrm{ff}\,x\,v)\,\mathrm{vol}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), ({\mathrm{ff}\,x\,v})'({\theta})={\mathrm{ff}^{\prime}\,x\,v\,\theta}) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \mathrm{AEStronglyMeasurable}\,(\mathrm{ff}^{\prime}\,x\,v)\,\mathrm{vol}) \to \forall (\mathrm{Bd} : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}} \to (\mathrm{Fin}\,4 \to \mathbb{R}) \to \mathbb{R}), (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}) (\theta : \mathbb{R}), \|\mathrm{ff}^{\prime}\,x\,v\,\theta\| \le \mathrm{Bd}\,x\,v) \to (\forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (v : \mathrm{Fin}\,4 \to \mathbb{R}), \href{/browser/qiqth-einsteinequationofstate#d-qiqth-einsteineos-bl}{({g\,x})({v},{v})} = 0 \to 2 \cdot \pi / \hbar \cdot {(\sum_{b} v\,b \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-pd}{\partial_{{b}}({\varphi})({x})})}^{2} = (-(2 \cdot \pi \cdot \int (\theta : \mathbb{R}), (\mathrm{starRingEnd}\,\mathbb{C})\,(\mathrm{ff}\,x\,v\,\theta) \cdot \mathrm{ff}^{\prime}\,x\,v\,\theta)).\mathrm{im}) \to \exists \Lambda, \forall (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{4}}}) (\mu \nu : \mathrm{Fin}\,4), a \cdot \href{/browser/qiqth-kgstressconservation#d-qiqth-curvature-kgstress}{T({x})\,\mu\,\nu} = \href{/browser/qiqth-curvature#d-qiqth-curvature-einsteintensor}{G_{{\mu}{\nu}}({x})} + \Lambda \cdot g_{{\mu}{\nu}}({x})

Proof. By qiqt_gr_freefield_nullEnergy. $\square$

Used by qiqt_gr_freefield_thermo.

← all sections · ← QiqtGrExplicitKG · QiqtGrGaussian →