CÁLCULO GRACELI SINTÉTICO [97]

G [f] t } G [s] = $\int _{s}^{\infty }F(\sigma )\,d\sigma \$ ] [ω] $i\omega e^{i\omega t}$ $\psi ^{*}$ ${\boldsymbol {\mu }}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] dx

G [f] t } G [s] = $\int _{s}^{\infty }F(\sigma )\,d\sigma \$ ] [ω] $i\omega e^{i\omega t}$ $\delta (x-\alpha )={\frac {1}{2\pi }}\int _{-\infty }^{\infty }e^{ip(x-\alpha )}\ dp\ .$

G f [t] [1/ ${\sqrt {2\pi }}$ ] [ω] $i\omega e^{i\omega t}$ ] $\lambda$ $\psi$ ${\hat {H}}$

G f [t] [1/ ${\sqrt {2\pi }}$ ] $i\omega e^{i\omega t}$ $\psi ^{*}$ ${\boldsymbol {\mu }}$ ] $\lambda$ ω ${\mathcal {T}}$ , $\sigma$ , $\psi$ $-i\hbar {\frac {\partial }{\partial x_{n}}}$ [x,t] ] dx

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CÁLCULO GRACELI SINTÉTICO [97]

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