Math 2.0

Relativity and gravitational theory Definition

Cosmological constant

Builds on Einstein field equationsEinstein tensorStress–energy tensor

Definition

Let (M,g)(M, g) be a four-dimensional Lorentzian manifold with Einstein tensor GG, carrying matter with stress–energy tensor TT. Let κ=8πGN/c4\kappa = 8\pi G_N / c^4, where GNG_N is Newton's gravitational constant and cc the speed of light. The cosmological constant is the real number Λ\Lambda in the Einstein field equations in the form Gμν+Λgμν=κTμν.G_{\mu\nu} + \Lambda g_{\mu\nu} = \kappa T_{\mu\nu}.

Remarks

Writing the term on the right gives Gμν=κ(Tμν+TμνΛ)G_{\mu\nu} = \kappa (T_{\mu\nu} + T^{\Lambda}_{\mu\nu}) with TΛ=−ΛκgT^\Lambda = -\frac{\Lambda}{\kappa} g. This is the stress–energy tensor of a perfect fluid with energy density ρΛ=Λ/κ\rho_\Lambda = \Lambda/\kappa and pressure pΛ=−ρΛp_\Lambda = -\rho_\Lambda, the vacuum energy. Example: de Sitter space with metric −dt2+e2Ht(dx2+dy2+dz2)-dt^2 + e^{2Ht}(dx^2 + dy^2 + dz^2), in units with c=1c = 1 and H>0H > 0, satisfies Ric=3H2g\mathrm{Ric} = 3H^2 g and R=12H2R = 12H^2, so G=−3H2gG = -3H^2 g; it solves the equations with T=0T = 0 and Λ=3H2>0\Lambda = 3H^2 > 0. Non-example: a nonconstant function Λ(x)\Lambda(x) in place of Λ\Lambda is not allowed when ∇μTμν=0\nabla^\mu T_{\mu\nu} = 0: taking the divergence and using ∇μGμν=0\nabla^\mu G_{\mu\nu} = 0 gives ∂νΛ=0\partial_\nu \Lambda = 0.

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  1. Einstein field equations concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Cosmological_constant
About this page
Tag49KF84BM0V
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WritingW0 stub
MSC83C05, 83F05
DefinesCosmological constant
UsesEinstein field equations, Einstein tensor, Stress–energy tensor
Changed3 November 2026

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