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General relativistic polytropes with a repulsive cosmological constant

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F47813059%3A19240%2F16%3AN0000028" target="_blank" >RIV/47813059:19240/16:N0000028 - isvavai.cz</a>

  • Result on the web

    <a href="http://journals.aps.org/prd/abstract/10.1103/PhysRevD.94.103513" target="_blank" >http://journals.aps.org/prd/abstract/10.1103/PhysRevD.94.103513</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1103/PhysRevD.94.103513" target="_blank" >10.1103/PhysRevD.94.103513</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    General relativistic polytropes with a repulsive cosmological constant

  • Original language description

    Spherically symmetric equilibrium configurations of perfect fluid obeying a polytropic equation of state are studied in spacetimes with a repulsive cosmological constant. The configurations are specified in terms of three parameters - the polytropic index $n$, the ratio of central pressure and central energy density of matter $sigma$, and the ratio of energy density of vacuum and central density of matter $lambda$. The static equilibrium configurations are determined by two coupled first-order nonlinear differential equations that are solved by numerical methods with the exception of polytropes with $n = 0$ corresponding to the configurations with a uniform distribution of energy density, when the solution is given in terms of elementary functions. The geometry of the polytropes is conveniently represented by embedding diagrams of both the ordinary space geometry and the optical reference geometry reflecting some dynamical properties of the geodesic motion. The polytropes are represented by radial profiles of energy density, pressure, mass, and metric coefficients. For all tested values of $n > 0$, the static equilibrium configurations with fixed parameters $n$, $sigma$, are allowed only up to a critical value of the cosmological parameter $lamda_c = lambda_c (n, σ)$. In the case of $n > 3$, the critical value $lambda_c$ tends to zero for special values of $sigma$. The gravitational potential energy and the binding energy of the polytropes are determined and studied by numerical methods. We discuss in detail the polytropes with an extension comparable to those of the dark matter halos related to galaxies, i.e., with extension $l >100 kpc$ and mass $M > 10^{12} M_{circle dot}$. For such largely extended polytropes, the cosmological parameter relating the vacuum energy to the central density has to be larger than $lambda = rho_{vac}/rho_c ∼ 10^{-9}$.

  • Czech name

  • Czech description

Classification

  • Type

    J<sub>x</sub> - Unclassified - Peer-reviewed scientific article (Jimp, Jsc and Jost)

  • CEP classification

    BN - Astronomy and celestial mechanics, astrophysics

  • OECD FORD branch

Result continuities

  • Project

    <a href="/en/project/GB14-37086G" target="_blank" >GB14-37086G: Albert Einstein Center for Gravitation and Astrophysics</a><br>

  • Continuities

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

Others

  • Publication year

    2016

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Name of the periodical

    Physical Review D

  • ISSN

    2470-0010

  • e-ISSN

  • Volume of the periodical

    94

  • Issue of the periodical within the volume

    10

  • Country of publishing house

    US - UNITED STATES

  • Number of pages

    37

  • Pages from-to

    '103513-1'-'103513-37'

  • UT code for WoS article

    000394505600003

  • EID of the result in the Scopus database

    2-s2.0-84995469163