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JHEP02(2005)050 doi: 10.1088/1126-6708/2005/02/050
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Abstract. Applying the first law of thermodynamics to the apparent horizon of a Friedmann-Robertson-Walker universe and assuming the geometric entropy given by a quarter of the apparent horizon area, we derive the Friedmann equations describing the dynamics of the universe with any spatial curvature. Using entropy formulae for the static spherically symmetric black hole horizons in Gauss-Bonnet gravity and in more general Lovelock gravity, where the entropy is not proportional to the horizon area, we are also able to obtain the Friedmann equations in each gravity theory. We also discuss some physical implications of our results.
Key words: Black Holes; Cosmology of Theories beyond the SM
Received 10 January 2005, accepted for publication 14 February 2005| Post to CiteUlike | | Post to Connotea | | Post to Bibsonomy |
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