EQUAÇÕES DE GRACELI

[

{\frac {\pi }{2}}t^{2}

] dt $[pk] n!, ] [$

\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}

\zeta (s)

/ [

\pi

/ pk]

{\mathcal {W}}\{f(t)\}\;=\;W(\omega ,\tau )\;=\;\int _{-\infty }^{\infty }f\left(\tau +{\frac {t}{2}}\right)\cdot f^{*}\left(\tau -{\frac {t}{2}}\right)\cdot e^{-i\omega t}\;dt\qquad (1a)

[

{\frac {\pi }{2}}t^{2}

] dt $[pk] n!, ] [$

\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}

\zeta (s)

/ [

\pi

/ pk]

f(t)\;=\;{\mathcal {W}}^{-1}\{W(\omega ,\tau )\}\;=\;{\frac {1}{2\pi \cdot f^{*}(0)}}\int _{-\infty }^{\infty }W\left(\omega ,{\frac {\tau }{2}}\right)\cdot e^{i\omega \tau }\;d\omega \qquad (1b)

^[1]^[2]

[

{\frac {\pi }{2}}t^{2}

] dt $[pk] n!, ] [$

\ln(n!)=\sum _{{k=1}}^{n}{\ln(k)}

\zeta (s)

/ [

\pi

/ pk]