CÁLCULO GRACELI SINTÉTICO [110]

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

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

f [x] [ ${\frac {\omega }{2\pi }}$ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ [ $-\;ie^{-ix}$ ] =

f [x] [ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ [ $-\;ie^{-ix}$ ] =

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

f [x] $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ [ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ =

f [x] ${\frac {1}{2\pi }}F(\omega )$ [ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ =

f [x] e−x2 [ ${\frac {\omega }{2\pi }}$ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ [ $-\;ie^{-ix}$ ] dx =

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

e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ dx =

f[x] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ dx =

f[x] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ dx =

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

f x[] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ [ $-\;ie^{-ix}$ ] dx =

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

f [x] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ dx =

f [x] e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ e−x2 [ ${\frac {\omega }{2\pi }}$ . $\pi \delta (x)$ ${\frac {1}{2\pi }}F(\omega )$ dx =

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CÁLCULO GRACELI SINTÉTICO [110]

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