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  <blog_url>https://www.mynote-jp.com/</blog_url>
  <categories>
    <anon>物理学</anon>
    <anon>物理学-電磁気学</anon>
    <anon>物理学-物理数学</anon>
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  <description>記法 電場 パルス $G_{2}(\tau)$ 参考文献 【関連記事】 時間平均 - Notes_JP 記法$g(t)$のフーリエ変換\begin{aligned} \mathcal{F}[g](\Omega) &amp;=\int_{-\infty}^{\infty} g(t) e^{-i\Omega t} \,\mathrm{d}t \end{aligned}$g(\Omega)$のフーリエ逆変換\begin{aligned} \mathcal{F}^{-1}[g](t) &amp;=\frac{1}{2\pi} \int_{-\infty}^{\infty} g(\Omega) e^{i\Omega t…</description>
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  <provider_name>Hatena Blog</provider_name>
  <provider_url>https://hatena.blog</provider_url>
  <published>2015-09-01 00:00:00</published>
  <title>電場の複素表示</title>
  <type>rich</type>
  <url>https://www.mynote-jp.com/entry/complex-representation-of-the-electric-field</url>
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