RicciSymm · section of the QIQT-H book

QIQTH.RicciSymm

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RicciSymm · entries 584–585 of 1000

Lemma 584 (lowered_riemann_pair_symm).  source ↗

Pair-symmetry of the lowered Riemann tensor R_{abcd} = R_{cdab} (with R_{pqrs} = ∑α g_{pα}R^α_{qrs}). The classical algebraic consequence of: first-pair antisymmetry (lowered_riemann_antisymm), last-pair antisymmetry (riemann_antisymm), and the first Bianchi identity (riemann_first_bianchi). Proof: sum the Bianchi identity over the four cyclic first-index placements; the cross terms cancel by the antisymmetries, leaving 2(R_{abcd} − R_{cdab}) = 0.

((y:Mn)(ab:Finn),gab(y)=gba(y))((y:Mn)(ab:Finn),σgaσ(y)gσb(y)=δab)((ab:Finn),(λygab(y))C)((abc:Finn),(λyΓbca(y))C)(abcd:Finn)(x:Mn),αgaα(x)Riemggiαbcdx=αgcα(x)Riemggiαdabx(\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}) (a b : \mathrm{Fin}\,n), g_{{a}{b}}({y}) = g_{{b}{a}}({y})) \to (\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}) (a b : \mathrm{Fin}\,n), \sum_{\sigma} g_{{a}{\sigma}}({y}) \cdot g^{{\sigma}{b}}({y}) = \delta_{ab}) \to (\forall (a b : \mathrm{Fin}\,n), ({\lambda y \mapsto g_{{a}{b}}({y})})\in C^{\infty}) \to (\forall (a b c : \mathrm{Fin}\,n), ({\lambda y \mapsto \href{/browser/qiqth-curvature#d-qiqth-curvature-christoffel}{\Gamma^{{a}}_{{b}{c}}({y})}})\in C^{\infty}) \to \forall (a b c d : \mathrm{Fin}\,n) (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}), \sum_{\alpha} g_{{a}{\alpha}}({x}) \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-riemann}{\mathrm{Riem}}\,g\,\mathrm{gi}\,\alpha\,b\,c\,d\,x = \sum_{\alpha} g_{{c}{\alpha}}({x}) \cdot \href{/browser/qiqth-curvature#d-qiqth-curvature-riemann}{\mathrm{Riem}}\,g\,\mathrm{gi}\,\alpha\,d\,a\,b\,x

Proof. By riemann_antisymm, riemann_first_bianchi, lowered_riemann_antisymm. \square

Used by ricci_symm.

Lemma 585 (ricci_symm).  source ↗

Ricci symmetry R_{σν} = R_{νσ} — discharges hric_symm. Write the Ricci tensor as the gi-raised lowered-Riemann trace (ricci_eq_trace), apply the pair-symmetry of the lowered Riemann (lowered_riemann_pair_symm) termwise, then reconcile by Finset.sum_comm + symmetry of gi.

((y:Mn)(ab:Finn),gab(y)=gba(y))((y:Mn)(ab:Finn),gab(y)=gba(y))((y:Mn)(ab:Finn),σgaσ(y)gσb(y)=δab)((ab:Finn),(λygab(y))C)((abc:Finn),(λyΓbca(y))C)(σν:Finn)(x:Mn),Rσν(x)=Rνσ(x)(\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}) (a b : \mathrm{Fin}\,n), g_{{a}{b}}({y}) = g_{{b}{a}}({y})) \to (\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}) (a b : \mathrm{Fin}\,n), g^{{a}{b}}({y}) = g^{{b}{a}}({y})) \to (\forall (y : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}) (a b : \mathrm{Fin}\,n), \sum_{\sigma} g_{{a}{\sigma}}({y}) \cdot g^{{\sigma}{b}}({y}) = \delta_{ab}) \to (\forall (a b : \mathrm{Fin}\,n), ({\lambda y \mapsto g_{{a}{b}}({y})})\in C^{\infty}) \to (\forall (a b c : \mathrm{Fin}\,n), ({\lambda y \mapsto \href{/browser/qiqth-curvature#d-qiqth-curvature-christoffel}{\Gamma^{{a}}_{{b}{c}}({y})}})\in C^{\infty}) \to \forall (\sigma \nu : \mathrm{Fin}\,n) (x : \href{/browser/qiqth-curvature#d-qiqth-curvature-point}{M^{{n}}}), \href{/browser/qiqth-curvature#d-qiqth-curvature-ricci}{R_{{\sigma}{\nu}}({x})} = \href{/browser/qiqth-curvature#d-qiqth-curvature-ricci}{R_{{\nu}{\sigma}}({x})}

Proof. By riemann, lowered_riemann_pair_symm. \square

Used by qiqt_bekenstein_gives_gr.


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