| Campo DC | Valor | Idioma |
| dc.contributor.author | Borges, H. A. | - |
| dc.contributor.author | Carneiro, Saulo | - |
| dc.contributor.author | Fabris, J. C. | - |
| dc.contributor.author | Zimdahl, W. | - |
| dc.creator | Borges, H. A. | - |
| dc.creator | Carneiro, Saulo | - |
| dc.creator | Fabris, J. C. | - |
| dc.creator | Zimdahl, W. | - |
| dc.date.accessioned | 2014-09-09T16:01:05Z | - |
| dc.date.issued | 2013 | - |
| dc.identifier.issn | 0370-2693 | - |
| dc.identifier.uri | http://repositorio.ufba.br/ri/handle/ri/15983 | - |
| dc.description | Texto completo: acesso restrito. p. 37–42 | pt_BR |
| dc.description.abstract | The split of a generalised Chaplygin gas with an equation of state p=−A/ραp=−A/ρα into an interacting mixture of pressureless matter and a dark-energy component with equation of state pΛ=−ρΛpΛ=−ρΛ implies the existence of non-adiabatic pressure perturbations. We demonstrate that the square of the effective (non-adiabatic) sound speed cscs of the medium is proportional to the ratio of the perturbations of the dark energy to those of the dark matter. Since, as demonstrated explicitly for the particular case α=−1/2α=−1/2, dark-energy perturbations are negligible compared with dark-matter perturbations on scales that are relevant for structure formation, we find View the MathML source|cs2|≪1. Consequently, there are no oscillations or instabilities which have plagued previous adiabatic Chaplygin-gas models. | pt_BR |
| dc.language.iso | en | pt_BR |
| dc.rights | Acesso Aberto | pt_BR |
| dc.source | http://dx.doi.org/10.1016/j.physletb.2013.10.032 | pt_BR |
| dc.title | Non-adiabatic Chaplygin gas | pt_BR |
| dc.title.alternative | Physics Letters B | pt_BR |
| dc.type | Artigo de Periódico | pt_BR |
| dc.identifier.number | v. 727, n. 1-3 | pt_BR |
| dc.embargo.liftdate | 10000-01-01 | - |
| Aparece nas coleções: | Artigo Publicado em Periódico (FIS)
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