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de Sitter space and Holography

de Sitter space and Holography

de Sitter space and Holography

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In d dimensions the Einstein equations with positivecosmological constant can be <strong>de</strong>rived from the actionI= I bulk + I GH∫1− d d x √ −g(R + 2Λ) + 116πG8πGM∫∂Md d−1 x √ hKhere• I GH is Gibbons-Hawking surface term which is nee<strong>de</strong>d toget a well-<strong>de</strong>fined Euler-Lagrange variation.• M is d-dimensional Manifold with Newton’s constant Gwith spatial Eucli<strong>de</strong>an boundary ∂M.• g µν is the bulk metric.• h µν <strong>and</strong> K are induced metric <strong>and</strong> the trace of the extrinsiccurvature of the boundary. The extrinsic curvature is <strong>de</strong>finedby K µν = −∇ (µ n ν) where n ν is outward pointing unit vector.• A useful length scale in the mo<strong>de</strong>l is given byl =√(d − 1)(d − 2)2ΛFor example in the vacuum dS solution, l is the radius of dS<strong>space</strong>.32

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