MECÂNICA GRACELI GENERALIZADA - QUÂNTICA DIMENSIONAL TENSORIAL RELATIVISTA DE CAMPOS [1.327]

1 / $\hbar$ $\psi$ 1 / $\hbar$ $\psi$ G $T^{\nu }{}_{\alpha }$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

1 / $G$ * = $\hbar$ $\psi$ $G$ * = $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ 1 / $\hbar$ $\psi$ $T^{\mu \nu }$ $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$

1 / $G$ * = $\hbar$ $\psi$ $G$ * = $= [$ 1 / $\hbar$ $\psi$ ] $\left|\psi ({\vec {r}},t)\right\rangle$ 1 / $\hbar$ $\psi$ $d$ $\left|\psi ({\vec {r}},t)\right\rangle$

1 / $G$ * = $\hbar$ $\psi$ $G$ * = $G_{\mu \nu }\$ 1 / $\hbar$ $\psi$ ${\hat {H}}$ $G$ * $F^{\mu \nu }$ $T_{\mu \nu }$ $d$ $\left|\psi ({\vec {r}},t)\right\rangle$

February 04, 2025

1 / $\hbar$ $\psi$ $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [ $\psi ^{*}$ 1 / $\hbar$ $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

1 / $G$ * = $\hbar$ $\psi$ $G$ * = 1 / $\hbar$ $\psi$ $[$ [ $\psi ^{*}$ 1 / $\hbar$ $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$

1 / $G$ * = $\hbar$ $\psi$ $G$ * = 1 / $\hbar$ $\psi$ $[$ [ $\psi ^{*}$ 1 / $\hbar$ $\psi$ $\left|\psi ({\vec {r}},t)\right\rangle$

1/ $G$ * = $\hbar$ $\psi$ 1 / $\hbar$ $\psi$ $\hbar$ 1 / $\hbar$ $\psi$ $\left|\psi ({\vec {r}},t)\right\rangle$

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MECÂNICA GRACELI GENERALIZADA - QUÂNTICA DIMENSIONAL TENSORIAL RELATIVISTA DE CAMPOS [1.327]

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