Abstract
AbstractWe have investigated the structural properties of strange quark stars (SQSs) in a modified theory of gravity known as massive gravity. In order to obtain the equation of state (EOS) of strange quark matter, we have employed a modified version of the Nambu–Jona-Lasinio model (MNJL) which includes a combination of NJL Lagrangian and its Fierz transformation by using weighting factors $$(1-\alpha )$$
(
1
-
α
)
and $$\alpha .$$
α
.
Additionally, we have also calculated dimensionless tidal deformability $$(\Lambda )$$
(
Λ
)
in massive gravity. To constrain the allowed values of the parameters appearing in massive gravity, we have imposed the condition $$\Lambda _{1.4 {M}_{\odot }}\lesssim 580 .$$
Λ
1.4
M
⊙
≲
580
.
Notably, in the MNJL model, the value of $$\alpha $$
α
varies between zero and one. As $$\alpha $$
α
increases, the EOS becomes stiffer, and the value of $$\Lambda $$
Λ
increases accordingly. We have demonstrated that by softening the EOS with increasing the bag constant, one can obtain objects in massive gravity that not only satisfy the constraint $$\Lambda _{1.4 {M} _{\odot }}\lesssim 580,$$
Λ
1.4
M
⊙
≲
580
,
but they also fall within the unknown mass gap region $$(2.5{M}_{\odot }-5{M}_{\odot }).$$
(
2.5
M
⊙
-
5
M
⊙
)
.
To establish that the obtained objects in this region are not black holes, we have calculated Schwarzschild radius, compactness, and $$\Lambda _{{M_{TOV}}}$$
Λ
M
TOV
in massive gravity.
Publisher
Springer Science and Business Media LLC
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