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Quantum Vacuum on the Worldline

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The <str<strong>on</strong>g>Quantum</str<strong>on</strong>g> <str<strong>on</strong>g>Vacuum</str<strong>on</strong>g><br />

<strong>Worldline</strong> Approach<br />

<strong>Worldline</strong> applicati<strong>on</strong>s<br />

Heisenberg-Euler effective acti<strong>on</strong>.<br />

Topography of QFT<br />

A view <strong>on</strong> <strong>the</strong> quantum vacuum<br />

Effective acti<strong>on</strong><br />

(EULER, KOCKEL’35; HEISENBERG, EULER’36;WEISSKOPF’36; SCHWINGER’51; RITUS’76)<br />

⊲ weak-field expansi<strong>on</strong><br />

Γ =<br />

<br />

−F + 8 α<br />

45<br />

2<br />

m4 F 2 + 14 α<br />

45<br />

2<br />

m4 G2 + O(F 6 )<br />

= + + . . .<br />

C<strong>on</strong>venti<strong>on</strong>s: F = 1<br />

4 FµνF µν = 1<br />

2 (B2 − E 2 ), G = 1<br />

4 Fµν ˜ F µν = −B · E<br />

Holger Gies <str<strong>on</strong>g>Quantum</str<strong>on</strong>g> <str<strong>on</strong>g>Vacuum</str<strong>on</strong>g> <strong>on</strong> <strong>the</strong> <strong>Worldline</strong>

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