Probing geometrically perturbed strange stars with minimal decoupling using millisecond pulsar timing observations

Abstract

We construct a gravitationally decoupled anisotropic strange star model using the minimal geometric deformation approach with a MIT bag equation of state and an additional source sector controlled by a deformation parameter β and a radial perturbation scale through g(r)=( r2). The resulting Einstein system is consistently split into seed and θ-sectors and matched to an exterior Schwarzschild geometry. The model is constrained by high-mass pulsars: PSR J0740+6620 (2.080.07\,M), PSR J1810+1744 (2.130.04\,M), PSR J1959+2048 (2.180.09\,M), and PSR J2215+5135 (2.28+0.10-0.09\,M). It reproduces these objects with predicted radii R ≈ 11.3--12.9 km. The maximum mass reaches M ≈ 2.28\,M for β = 3× 10-3 and ≈ 0.03\,km-2, while for β = 10-3 the configuration yields M ≈ 2.12\,M with R ≈ 12.2 km. The central density lies in c ≈ (2.4--3.1)× 10-4\,km-2, decreasing smoothly to s ≈ 2.0× 10-4\,km-2. The anisotropy increases from zero at the center to ≈ (0.25--0.45)× 10-4\,km-2 near the surface, generating additional outward support that enhances compactness by 15\%. The compactness parameter spans C ≈ 0.17--0.22, safely below the Buchdahl limit, while the surface redshift reaches zs ≈ 0.25--0.38. The condition dM/dc > 0 is satisfied throughout, confirming dynamical stability. Overall, β enhances the maximum mass by up to 15\%, while introduces controlled oscillatory structure without violating observational constraints, producing stable ultra-compact stars consistent with current pulsar data.

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