Please use this identifier to cite or link to this item: http://dspace.iitrpr.ac.in:8080/xmlui/handle/123456789/1129
Full metadata record
DC FieldValueLanguage
dc.contributor.authorBhattacharya, S.-
dc.contributor.authorKousvos, S.R.-
dc.contributor.authorRomanopoulos, S.-
dc.contributor.authorTomaras, T.N.-
dc.date.accessioned2018-12-29T06:32:38Z-
dc.date.available2018-12-29T06:32:38Z-
dc.date.issued2018-12-29-
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/1129-
dc.description.abstractThe scalar and vector cosmological perturbations at all length scales of our Universe are studied in the framework of the phantom braneworld model. The model is characterized by the parameter M ≡ M3/2m2H0, with M and m the five- and four-dimensional Planck scales, respectively, and H0 the Hubble parameter today, while M → 0 recovers the CDM model. Ignoring the backreaction due to the peculiar velocities and also the bulk cosmological constant, allows the explicit computation of the gravitational potentials, and . They exhibit exponentially decreasing screening behaviour characterized by a screening length which is a function of the quasidensity parameter M .en_US
dc.language.isoen_USen_US
dc.titleCosmological screening and the phantom braneworld modelen_US
dc.typeArticleen_US
Appears in Collections:Year-2018

Files in This Item:
File Description SizeFormat 
Full Text.pdf793.96 kBAdobe PDFView/Open    Request a copy


Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.