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Manuscript X-E-ST@1 · X-E-ST.tex · section · 44614221

Feynman-weight de Donder gauge fixing

E3: the derived free graviton operator › Feynman-weight de Donder gauge fixing · lines 1075–1086

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Define

(P_{tr} l)_{μν} = l_{μν} - \frac{1}{2} η_{μν} tr_{η} l, C^{μ} [l] = \partial_{ν} (P_{tr} l)^{ν μ}, S_{gf} [l] = \frac{1}{4} \int C_{μ} [l] C^{μ} [l] d^{4} x .

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unlabeled · line 1078
$(P_{tr} l)_{μν} = l_{μν} - \frac{1}{2} η_{μν} tr_{η} l, C^{μ} [l] = \partial_{ν} (P_{tr} l)^{ν μ}, S_{gf} [l] = \frac{1}{4} \int C_{μ} [l] C^{μ} [l] d^{4} x .$

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