Gravity as elasticity of spacetime: A paradigm to understand horizon thermodynamics and cosmological constant

dc.contributor.authorPadmanabhan, T.
dc.date.accessioned2012-03-03T15:14:11Z
dc.date.available2012-03-03T15:14:11Z
dc.date.issued2004-05-20
dc.description.abstractIt is very likely that the quantum description of spacetime is quite di erent from what we perceive at large scales, l (G~=c3)1=2. The long wavelength description of spacetime, based on Einstein's equations, is similar to the description of a continuum solid made of a large number of microscopic degrees of freedom. This paradigm provides a novel interpretation of coordinate transformations as deformations of \spacetime solid" and allows one to obtain Einstein's equations as a consistency condition in the long wave- length limit. The entropy contributed by the microscopic degrees of freedom reduces to a pure surface contribution when Einstein's equations are satis ed. The horizons arises as \defects" in the \spacetime solid" (in the sense of well-de ned singular points) and contributes an entropy which is one quarter of the horizon area. Finally, the response of the microstructure to vacuum energy leads to a near cancellation of the cosmological constant, leaving behind a tiny uctuation which matches with the observed value.en_US
dc.identifier.urihttp://hdl.handle.net/11007/225
dc.language.isoenen_US
dc.publisherWorld Scientific Publishing Companyen_US
dc.relation.ispartofseriesInternational Journal of Modern Physics D;Vol. 13, No. 10, 2004
dc.subjectHorizonen_US
dc.subjectEntropyen_US
dc.subjectBlack holeen_US
dc.subjectCosmological constanten_US
dc.subjectQuantum gravityen_US
dc.titleGravity as elasticity of spacetime: A paradigm to understand horizon thermodynamics and cosmological constanten_US
dc.typeArticleen_US

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