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Cosmological Principle

The Cosmological Principle assumes that the universe is homogeneous and isotropic on large scales, meaning it looks the same in all directions and locations.
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The statement of the theorem

The Cosmological Principle assumes that the universe is statistically homogeneous and isotropic on sufficiently large scales. Mathematically, this implies that the metric tensor gμνg_{\mu\nu} can be written in the Friedmann-Lemaître-Robertson-Walker (FLRW) form, which depends only on time tt and the scale factor a(t)a(t), but not on the spatial coordinates (x,y,z)(x, y, z): \n\nds2=c2dt2+a2(t)[dr21kr2+r2(dθ2+sin2θdϕ2)]ds^2 = -c^2 dt^2 + a^2(t) \left[ \frac{dr^2}{1 - k r^2} + r^2 (d\theta^2 + \sin^2\theta d\phi^2) \right]\n\nWhere kk is the spatial curvature parameter.