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Display information for equation id:math.1199.674 on revision:1199

* Page found: Elektrodynamik Schöll (eq math.1199.674)

Occurrences on the following pages:

Retardierte Potenziale Eq: math.2129.28

Hash: ac39c3dd37158d419750fc6d0d031699

TeX (original user input):

\Gamma (\bar{q},\tau ):=\int_{-\infty }^{\infty }{d\omega }\frac{{{e}^{-i\omega \tau }}}{\left( {{q}^{2}}-\frac{{{\omega }^{2}}}{{{c}^{2}}} \right)}=\oint\limits_{C}{d\omega }\frac{{{e}^{-i\omega \tau }}}{\left( {{q}^{2}}-\frac{{{\omega }^{2}}}{{{c}^{2}}} \right)}=2\pi i\sum\limits_{Pole}^{{}}{{}}\operatorname{Re}s\frac{{{e}^{-i\omega \tau }}}{\left( {{q}^{2}}-\frac{{{\omega }^{2}}}{{{c}^{2}}} \right)}

TeX (checked):

\Gamma ({\bar {q}},\tau ):=\int _{-\infty }^{\infty }{d\omega }{\frac {{e}^{-i\omega \tau }}{\left({{q}^{2}}-{\frac {{\omega }^{2}}{{c}^{2}}}\right)}}=\oint \limits _{C}{d\omega }{\frac {{e}^{-i\omega \tau }}{\left({{q}^{2}}-{\frac {{\omega }^{2}}{{c}^{2}}}\right)}}=2\pi i\sum \limits _{Pole}^{}{}\operatorname {Re} s{\frac {{e}^{-i\omega \tau }}{\left({{q}^{2}}-{\frac {{\omega }^{2}}{{c}^{2}}}\right)}}

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Γ (\bar{q}, τ) : = \int_{- \infty}^{\infty} d ω \frac{e^{- i ω τ}}{(q^{2} - \frac{ω^{2}}{c^{2}})} = \oint_{C} d ω \frac{e^{- i ω τ}}{(q^{2} - \frac{ω^{2}}{c^{2}})} = 2 π i \sum_{P o l e}^{} ℜ s \frac{e^{- i ω τ}}{(q^{2} - \frac{ω^{2}}{c^{2}})}

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Identifiers

$Γ$

$\bar{q}$

$τ$

$ω$

$e$

$i$

$ω$

$τ$

$q$

$ω$

$c$

$C$

$d$

$ω$

$e$

$i$

$ω$

$τ$

$q$

$ω$

$c$

$π$

$i$

$P$

$o$

$l$

$e$

$s$

$e$

$i$

$ω$

$τ$

$q$

$ω$

$c$

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