Cosmological exact solutions of Petrov type D of a nonlinear asymptotic fluid to a dark energy fluid in real and complex geometries with double singularity. Second case.
{"title":"Cosmological exact solutions of Petrov type D of a nonlinear asymptotic fluid to a dark energy fluid in real and complex geometries with double singularity. Second case.","authors":"R. Alvarado","doi":"10.12988/astp.2021.91675","DOIUrl":null,"url":null,"abstract":"Abstract In this paper, exact solutions to the Einstein’s equations are obtained for an anisotropic and homogeneous symmetry of Petrov Type D from a nonlinear fluid that responds to the equation of state Q+Q− = 0 where Q± = √ μ1 (−2P1 + μ1) ± 2 BP1 a wherein μ1 = μ − Λ, P1 = P + Λ, and μ, P and Λ are the volumetric energy density, the pressure, and a constant linked to the concept of dark energy. That equation of state and what it represents in certain limits of time (when t→ 0 and when t → ∞) are also analyzed. Two general solutions which are different because of the degree of initial expansion that a coordinate can have in relation to a perpendicular plane are obtained. For each solution, two cases are present: one represents a space-time with real geometry (R) for all the values of t, and asymptotically in time, this case becomes an isotropic space-time of FLRW of a dark energy fluid; and the other one presents a double singularity, so that since the first singularity, space-time is complex (C) until a certain time t = a ( when the second singularity is present) from which space-time is real (R) and with the increase of time, it tends to an isotropic space-time of FLRW from a dark energy fluid. Then, temperature behavior in relation to time is obtained.","PeriodicalId":127314,"journal":{"name":"Advanced Studies in Theoretical Physics","volume":"36 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Studies in Theoretical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.12988/astp.2021.91675","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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Abstract
Abstract In this paper, exact solutions to the Einstein’s equations are obtained for an anisotropic and homogeneous symmetry of Petrov Type D from a nonlinear fluid that responds to the equation of state Q+Q− = 0 where Q± = √ μ1 (−2P1 + μ1) ± 2 BP1 a wherein μ1 = μ − Λ, P1 = P + Λ, and μ, P and Λ are the volumetric energy density, the pressure, and a constant linked to the concept of dark energy. That equation of state and what it represents in certain limits of time (when t→ 0 and when t → ∞) are also analyzed. Two general solutions which are different because of the degree of initial expansion that a coordinate can have in relation to a perpendicular plane are obtained. For each solution, two cases are present: one represents a space-time with real geometry (R) for all the values of t, and asymptotically in time, this case becomes an isotropic space-time of FLRW of a dark energy fluid; and the other one presents a double singularity, so that since the first singularity, space-time is complex (C) until a certain time t = a ( when the second singularity is present) from which space-time is real (R) and with the increase of time, it tends to an isotropic space-time of FLRW from a dark energy fluid. Then, temperature behavior in relation to time is obtained.