Gravity as elasticity of spacetime: A paradigm to understand horizon thermodynamics and cosmological constant
| dc.contributor.author | Padmanabhan, T. | |
| dc.date.accessioned | 2012-03-03T15:14:11Z | |
| dc.date.available | 2012-03-03T15:14:11Z | |
| dc.date.issued | 2004-05-20 | |
| dc.description.abstract | It 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.uri | http://hdl.handle.net/11007/225 | |
| dc.language.iso | en | en_US |
| dc.publisher | World Scientific Publishing Company | en_US |
| dc.relation.ispartofseries | International Journal of Modern Physics D;Vol. 13, No. 10, 2004 | |
| dc.subject | Horizon | en_US |
| dc.subject | Entropy | en_US |
| dc.subject | Black hole | en_US |
| dc.subject | Cosmological constant | en_US |
| dc.subject | Quantum gravity | en_US |
| dc.title | Gravity as elasticity of spacetime: A paradigm to understand horizon thermodynamics and cosmological constant | en_US |
| dc.type | Article | en_US |