Constraining f(R) gravity by Pulsar SAX J1748.9-2021 observations
We discuss spherically symmetric dynamical systems in the framework of a general model of f ( R ) gravity, i.e. f ( R ) = R e ζ R , where ζ is a dimensional quantity in squared length units [L 2 ]. We initially assume that the internal structure of such systems is governed by the Krori–Barua ansatz,...
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Veröffentlicht in: | The European physical journal. C, Particles and fields Particles and fields, 2024-05, Vol.84 (5), p.521, Article 521 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We discuss spherically symmetric dynamical systems in the framework of a general model of
f
(
R
)
gravity, i.e.
f
(
R
)
=
R
e
ζ
R
, where
ζ
is a dimensional quantity in squared length units [L
2
]. We initially assume that the internal structure of such systems is governed by the Krori–Barua ansatz, alongside the presence of fluid anisotropy. By employing astrophysical observations obtained from the pulsar
S
AX J1748.9-2021, derived from bursting X-ray binaries located within globular clusters, we determine that
ζ
is approximately equal to
±
5
km
2
. In particular, the model is capable of producing stable configurations for
S
AX J1748.9-2021, encompassing both its geometric and physical characteristics. We show that, within the framework of
f
(
R
)
gravity, the Krori–Barua ansatz establishes semi-analytical connections between the radial (
p
r
) and tangential (
p
t
) pressures, and the density (
ρ
). These relations are described as
p
r
≈
v
r
2
(
ρ
-
ρ
I
)
and
p
t
≈
v
t
2
(
ρ
-
ρ
II
)
. In this context,
v
r
and
v
t
denote the sound speeds in the radial and tangential directions, respectively. Meanwhile,
ρ
I
pertains to the surface density, and
ρ
II
is derived from the model parameters. These connections are consistent with the equations of state derived from the best-fit solutions identified in the ongoing investigation. Notably, within the framework of
f
(
R
)
gravity where
ζ
is negative, the maximum compactness, denoted as
C
, is inherently limited to values that do not exceed the Buchdahl limit. This contrasts with general relativity or
f
(
R
)
gravity with
ζ
positive, where the compactness has the potential to asymptotically reach the black hole threshold (
C
→
1
). The model predictions suggest a central density that largely exceeds the saturation nuclear density, which is
ρ
nuc
=
3
×
10
14
g/cm
3
. Also the surface density
ρ
I
surpasses
ρ
nuc
. We obtain a mass-radius diagram, corresponding to the boundary density, which is consistent with other observational data. |
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ISSN: | 1434-6052 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-024-12866-8 |