CÁLCULO GRACELI SINTÉTICO [110]

$equação Graceli dimensional relativista tensorial quântica de campos$

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

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

$\psi ^{*}$

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f [x] ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] [ e−x2 [ ${\frac {\omega }{2\pi }}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] [ ${\frac {\omega }{2\pi }}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] [ e−x2 [ ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] ${\frac {1}{2\pi }}F(\omega )$ [ e−x2 [ ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ [ $-{\frac {\pi }{2}}$ ] ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f[x] e−x2 [ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f[x] e−x2 [ ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$

f [x] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ e−x2 [ ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω , $dx =$

f x[] ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω [ $-\;ie^{-ix}$ ] dx =

f [ x] ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω dx =

f [x] ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\frac {1}{2\pi }}F(\omega )$ dx =

f [x] ${\frac {1}{2\pi }}F(\omega )$ ${\frac {\omega }{2\pi }}$ .] $\lambda$ ω ${\frac {1}{2\pi }}F(\omega )$ dx =

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CÁLCULO GRACELI SINTÉTICO [110]

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