TRANSFORMADA QUÂNTICA E RELATIVISTA DE GRACELI

TRANSFORMADA RELATIVISTA E QUÂNTICA DE GRACELI.

F [ (λ) h ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ ] ]=F [f] [(λ) h ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ ]] = f [t] (λ) h ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ ] dt

F [ (λ) h ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ ] ] = f [t] [cos - i sin(λ) h ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ ] ] dt

F [ $E=mc^{2}$ ] = F [f] [ $E=mc^{2}$ ] = f [t] $E=mc^{2}$ dt

F [ $E=mc^{2}$ ] = f [t] [cos - i sin $E=mc^{2}$ ] dt

F [ $R_{\mu \nu }-{g_{\mu \nu }R \over 2}+\Lambda g_{\mu \nu }=8\pi {G \over c^{4}}T_{\mu \nu }$ de/dt.] = F [f] [ $R_{\mu \nu }-{g_{\mu \nu }R \over 2}+\Lambda g_{\mu \nu }=8\pi {G \over c^{4}}T_{\mu \nu }$ de/dt.] = f [t] $R_{\mu \nu }-{g_{\mu \nu }R \over 2}+\Lambda g_{\mu \nu }=8\pi {G \over c^{4}}T_{\mu \nu }$ de/dt. dt

F [ $R_{\mu \nu }-{g_{\mu \nu }R \over 2}+\Lambda g_{\mu \nu }=8\pi {G \over c^{4}}T_{\mu \nu }$ de/dt.] = f [t] [cos - i sin $R_{\mu \nu }-{g_{\mu \nu }R \over 2}+\Lambda g_{\mu \nu }=8\pi {G \over c^{4}}T_{\mu \nu }$ de/dt. ] dt

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TRANSFORMADA QUÂNTICA E RELATIVISTA DE GRACELI

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