DC FieldValueLanguage
dc.contributor.authorDimitrijevic, I.en
dc.contributor.authorDragovich, B.en
dc.contributor.authorRakic, Z.en
dc.contributor.authorStankovic, J.en
dc.date.accessioned2020-12-11T13:04:43Z-
dc.date.available2020-12-11T13:04:43Z-
dc.date.issued2019-09-01en
dc.identifier.issn00815438en
dc.identifier.urihttp://researchrepository.mi.sanu.ac.rs/handle/123456789/4437-
dc.description.abstract© 2019, Pleiades Publishing, Ltd. Significant phenomenological success and nice theoretical properties of general relativity (GR) are well known. However, GR is not a complete theory of gravity. Hence, there are many attempts to modify GR. One of the current approaches to a more complete theory of gravity is a nonlocal modification of GR. The nonlocal gravity approach, which we consider here without matter, is based on the action S=(16πG)−1∫−g(R−2Λ+P(R)ℱ(□)Q(R))d4x, where R is the scalar curvature, Γ is the cosmological constant, P(R) and Q(R) are some differentiable functions of R, and ℱ(□)=∑n=1+∞fn□n is an analytic function of the corresponding d’Alembert operator □. We present here a brief review of some general properties and cosmological solutions for some specific functions P(R) and Q(R).en
dc.relation.ispartofProceedings of the Steklov Institute of Mathematicsen
dc.titleCosmological Solutions of Some Nonlocal Gravity Modelsen
dc.typeArticleen
dc.identifier.doi10.1134/S0081543819050079en
dc.identifier.scopus2-s2.0-85077363414en
dc.identifier.urlhttps://api.elsevier.com/content/abstract/scopus_id/85077363414en
dc.relation.firstpage66en
dc.relation.lastpage73en
dc.contributor.orcid#NODATA#en
dc.contributor.orcid#NODATA#en
dc.contributor.orcid#NODATA#en
dc.contributor.orcid#NODATA#en
dc.relation.issue1en
dc.relation.volume306en
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.fulltextNo Fulltext-
item.grantfulltextnone-
item.openairetypeArticle-
item.cerifentitytypePublications-
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