CÁLCULO GRACELI SINTÉTICO [57]

$a_0$ f (z) = $a_n$ cos u [x , y] + $G_{\mu \nu }\$ $T_{\mu \nu }$ $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$ [ v [ x, y]] + $b_n$ sen u [x , y] + $G_{\mu \nu }\$ $T_{\mu \nu }$ $T^{\nu }{}_{\alpha }$ [DR] = ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$ $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ $.$ = $\left|\psi ({\vec {r}},t)\right\rangle$ [ v [ x, y]] =

$a_0$ f (z) = $a_n$ cos u [x , y] + $\psi ^{*}$ [ $\psi ^{*}$ ${\boldsymbol {\mu }}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] [ v [ x, y]] + $b_n$ sen u [x , y] + $\psi ^{*}$ [ $\psi ^{*}$ ${\boldsymbol {\mu }}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ][ v [ x, y]] =

$a_0$ f (z) = $a_n$ cos u [x , y] +

$G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $\eta _{\mu \nu }$ = [ v [ x, y]] + $b_n$ sen u [x , y] +

$G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$ [DR] = $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $\eta _{\mu \nu }$ =[ v [ x, y]] =

$a_0$ f (z) = $a_n$ cos u [x , y] + G $T^{\nu }{}_{\alpha }$ [DR] = $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $\eta _{\mu \nu }$ [ v [ x, y]] + $b_n$ sen u [x , y] + G $T^{\nu }{}_{\alpha }$ [DR] = $F^{\mu \nu }$ $T^{\mu \nu }$ $P^{\mu }\!$ $\eta _{\mu \nu }$ [ v [ x, y]] =

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CÁLCULO GRACELI SINTÉTICO [57]

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