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Thermodynamics of anomaly-driven cosmology

James E Lidsey

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NOTE

The Friedmann equations of general relativity can be derived from the first law of thermodynamics when the entropy of the apparent horizon of a spatially isotropic universe is given by the Bekenstein–Hawking entropy. We point out that if the entropy of the apparent horizon receives a logarithmic correction, the first law of thermodynamics leads to a modified Friedmann equation which corresponds precisely to the time–time component of the semi-classical Einstein field equations sourced by the trace anomaly of the {\cal{N}}=4, \, U(N) super-Yang–Mills theory. This correspondence allows for a thermodynamic description of the dynamics of the Randall–Sundrum braneworld scenario.


PACS

98.80.Cq Particle-theory and field-theory models of the early Universe (including cosmic pancakes, cosmic strings, chaotic phenomena, inflationary universe, etc.)

11.30.Pb Supersymmetry

04.70.Dy Quantum aspects of black holes, evaporation, thermodynamics

11.15.-q Gauge field theories

04.20.-q Classical general relativity

MSC

83F05 Cosmology

83C57 Black holes

82B30 Statistical thermodynamics (See also 80-XX)

81T13 Yang-Mills and other gauge theories (See also 53C07, 58E15)

85A40 Cosmology (For relativistic cosmology, see 83F05)

81T60 Supersymmetric field theories

Subjects

Gravitation and cosmology

Particle physics and field theory

Astrophysics and astroparticles

Dates

Issue 14 (21 July 2009)

Received 2 April 2009

Published 18 June 2009



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