Update 2022-02-08 17:21
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-02-08 Tue 06:55 -->
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<!-- 2022-02-08 Tue 17:21 -->
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<meta charset="utf-8">
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<meta name="viewport" content="width=device-width, initial-scale=1">
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<title>Pre-Quantum Electrodynamics</title>
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@@ -272,6 +272,10 @@ Table of contents
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</summary>
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<ul>
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<li>
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<a href="./in_t_l.html#in_t_l">Section and equation labelling</a><span class="headline-id">in.t.l</span>
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</li>
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<li>
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<a href="./in_t_c.html#in_t_c">Contextual colors</a><span class="headline-id">in.t.c</span>
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</li>
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@@ -736,7 +740,7 @@ Table of contents
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</li>
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<li>
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<a href="./emsm_esm_d.html#emsm_esm_d">Dielectrics</a><span class="headline-id">emsm.esm.d</span>
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<a href="./emsm_esm_di.html#emsm_esm_di">Dielectrics</a><span class="headline-id">emsm.esm.di</span>
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</li>
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<li>
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@@ -1688,7 +1692,7 @@ how the nonvanishing elements of an antisymmetric tensor transform:
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<p>
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Comparing with the transformation rules for the electromagnetic field which we obtained in (\ref{eq:EMFieldsLorentzTransfo}), we can define the
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</p>
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<div class="core div" id="orga725a53">
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<div class="core div" id="org59626ea">
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<p>
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{\bf Electromagnetic Field Tensor}
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\[
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@@ -1704,7 +1708,7 @@ Comparing with the transformation rules for the electromagnetic field which we o
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<p>
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together with the handy
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</p>
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<div class="main div" id="org14dbfc2">
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<div class="main div" id="org54e2473">
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<p>
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{\bf Dual Field Tensor}
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\[
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@@ -1728,7 +1732,7 @@ obtained from the field tensor by the substitution
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<p>
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Our electromagnetic field transformation laws then become the simple
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</p>
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<div class="core div" id="org8c48487">
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<div class="core div" id="org1eec6b9">
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<p>
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{\bf Lorentz Transformation Rules for EM Fields}
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\[
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@@ -1745,7 +1749,7 @@ Our electromagnetic field transformation laws then become the simple
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<hr><div id="postamble" class="status">
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<p class="author">Author: Jean-Sébastien Caux</p>
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<p class="date">Created: 2022-02-08 Tue 06:55</p>
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<p class="date">Created: 2022-02-08 Tue 17:21</p>
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<p class="validation"><a href="https://validator.w3.org/check?uri=referer">Validate</a></p>
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</div>
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