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The Einstein--Hilbert action, coupled to matter with Lagrangian density $\mathcal{L}_m$, is


\[

S = \frac{1}{2\kappa} \int_M R \sqrt{-g}\, \mathrm{d}^4x \;+\; \int_M \mathcal{L}_m \sqrt{-g}\, \mathrm{d}^4x,

\qquad \kappa = \frac{8\pi G}{c^4},

\]


where $R = g^{\mu\nu} R_{\mu\nu}$ is the Ricci scalar, $g = \det(g_{\mu\nu})$, and $R_{\mu\nu}$ is the Ricci tensor built from the Christoffel…

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