dc.contributor.author | Alexandre, J | en |
dc.contributor.author | Pasipoularides, P | en |
dc.date.accessioned | 2014-03-01T02:07:02Z | |
dc.date.available | 2014-03-01T02:07:02Z | |
dc.date.issued | 2011 | en |
dc.identifier.issn | 1550-7998 | en |
dc.identifier.uri | https://dspace.lib.ntua.gr/xmlui/handle/123456789/29513 | |
dc.subject.classification | Astronomy & Astrophysics | en |
dc.subject.classification | Physics, Particles & Fields | en |
dc.subject.other | COSMOLOGY | en |
dc.title | Spherically symmetric solutions, Newton's Law, and the infrared limit lambda -> 1 in covariant Horava-Lifshitz gravity | en |
heal.type | journalArticle | en |
heal.identifier.secondary | 084020 | en |
heal.language | English | en |
heal.publicationDate | 2011 | en |
heal.abstract | In this note we examine whether spherically symmetric solutions in covariant Horava-Lifshitz gravity can reproduce Newton's Law in the IR limit lambda -> 1. We adopt the position that the auxiliary field A is independent of the space-time metric [J. Alexandre and P. Pasipoularides, Phys. Rev. D 83, 084030 (2011).][J. Greenwald, V. H. Satheeshkumar, and A. Wang, J. Cosmol. Astropart. Phys. 12 (2010) 007.], and we assume, as in [A. M. da Silva, Classical Quantum Gravity 28, 055011 (2011).], that lambda is a running coupling constant. We show that under these assumptions, spherically symmetric solutions fail to restore the standard Newtonian physics in the IR limit lambda -> 1, unless lambda does not run, and has the fixed value lambda = 1. Finally, we comment on the Horava and Melby-Thompson approach [P. Horava and C. M. Melby-Thompson, Phys. Rev. D 82, 064027 (2010).] in which A is assumed as a part of the space-time metric in the IR. | en |
heal.publisher | AMER PHYSICAL SOC | en |
heal.journalName | PHYSICAL REVIEW D | en |
dc.identifier.isi | ISI:000296527800007 | en |
dc.identifier.volume | 84 | en |
dc.identifier.issue | 8 | en |
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