2015
DOI: 10.1088/1742-6596/615/1/012003
|View full text |Cite
|
Sign up to set email alerts
|

Static solutions of Einstein's field equations for compact stellar objects

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
23
1
1

Year Published

2017
2017
2021
2021

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 27 publications
(25 citation statements)
references
References 19 publications
0
23
1
1
Order By: Relevance
“…This result could be a consequence of the dependency of Q on gamma, which implies a direct dependency on the EoS and therefore, varies between the stars. This result is different from the one obtained in Zubairi et al (2015)), where structure equations derived from the γ metric were solved by taking γ as a free parameter set by hand. In that case, since the mass quadrupole is leaded by the mass, its highest values are reached for the more massive stars.…”
Section: Mass Quadrupole Momentcontrasting
confidence: 89%
“…This result could be a consequence of the dependency of Q on gamma, which implies a direct dependency on the EoS and therefore, varies between the stars. This result is different from the one obtained in Zubairi et al (2015)), where structure equations derived from the γ metric were solved by taking γ as a free parameter set by hand. In that case, since the mass quadrupole is leaded by the mass, its highest values are reached for the more massive stars.…”
Section: Mass Quadrupole Momentcontrasting
confidence: 89%
“…The case α = 0 corresponding to 5D GR is also shown for comparison reasons. We see that we obtain the usual profiles familiar from the standard four-dimensional GR, although the 5D objects are larger and much heavier than their 4D counterparts [49,50]. First, the radius acquires a maximum value, R max , while the star mass still increases.…”
Section: Numerical Resultsmentioning
confidence: 53%
“…This can be easily seen using the equations presented before valid in the Einstein frame (without matter P = 0 = ǫ) as follows. If we assume solutions with a constant value for the scalar field, φ = const = φ 0 , that in addition corresponds to an extremum of the potential, V ,φ (φ 0 ) = 0, then the two last equations are automatically satisfied, while the first two are essentially the tt and rr equations of GR with a cosmological constant Λ = V (φ 0 )/2 [56]. For the Starobinsky's model φ 0 = 0 = V (φ 0 ), and we thus obtain the anticipated Schwarzschild black hole solution.…”
Section: Numerical Resultsmentioning
confidence: 99%