CÁLCULO GRACELI SINTÉTICO [130]

INTEGRAL DE GRACELI.

f[x] = $\lambda$ ω Σa_nΣa_n] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $\Phi$ $f$ , $a(x,\xi )$ $\xi$

f[x] = $G* =$ $\lambda$ ω Σa_nΣa_n] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $f$ , $a(x,\xi )$ $\xi$

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ Σa_n] $\lambda$ ω , $\sigma$ , $\psi$ $f$ , $a(x,\xi )$ $\xi$

$f[x] =$ Σa_n $\lambda$ $f$ , $a(x,\xi )$ $\xi$

$f[x] =$ Σa_n $\psi ^{*}$ Σa_n $]$ $\psi ^{*}$ $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$

$f[x] =$ Σa_nΣa_n $]$ ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$

INTEGRAL DE GRACELI.

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $\Phi$ $f$ , $a(x,\xi )$ $\xi$

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $f$ , $a(x,\xi )$ $\xi$

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ ] $\lambda$ ω , $\sigma$ , $\psi$ $f$ , $a(x,\xi )$ $\xi$

$\psi ^{*}$ $f$ , $a(x,\xi )$ $\xi$

$\psi ^{*}$ $\psi ^{*}$ $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$

$\psi ^{*}$ ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$

INTEGRAL DE GRACELI.

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $\Phi$ $f$ , $a(x,\xi )$ $\xi$

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $f$ , $a(x,\xi )$ $\xi$

f[x] = $\psi ^{*}$ $f$ , $a(x,\xi )$ ] $\lambda$ ω , $\sigma$ , $\psi$ $f$ , $a(x,\xi )$ $\xi$

$\psi ^{*}$ $f$ , $a(x,\xi )$ $\xi$

$\psi ^{*}$ $\psi ^{*}$ $G_{\mu \nu }\$ $T_{\mu \nu }$ G $T^{\nu }{}_{\alpha }$

$\psi ^{*}$ ${\hat {H}}$ $\left|\psi ({\vec {r}},t)\right\rangle$