MECÂNICA GRACELI GENERALIZADA - QUÂNTICA TENSORIAL DIMENSIONAL RELATIVISTA DE CAMPOS [1.199]

FUNÇÃO G DE GRACELI.

- ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

G = E dt [G]

- ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

G = E dt [G].

- ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $\psi ^{*}$

G = E $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$ [G]

- ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $\psi ^{*}$ $G* ]$

G = E $T_{\mu \nu }$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$ [G]