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Exploring compact stars in modified <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si12.svg"> <mml:mrow> <mml:mi>f</mml:mi> <mml:mo>(</mml:mo> <mml:mi mathvariant="script">G</mml:mi> <mml:mo>,</mml:mo> <mml:mi>φ</mml:mi> <mml:mo>)</mml:mo> </mml:mrow> </mml:math> gravity

Zoya AsgharNational University of Computer and Emerging Sciences, Lahore Campus, PakistanM. Farasat ShamirCenter for Theoretical Physics, Khazar University, 41 Mehseti Str., Baku, AZ1096, AzerbaijanFatemah MofarrehMathematical Science Department, College of Science, Princess Nourah Bint Abdulrahman University, Riyadh, 11546, Saudi ArabiaJavlon RayimbaevInstitute of Fundamental and Applied Research, National Research University TIIAME, Kori Niyoziy 39, Tashkent, 100000, UzbekistanOtaboyev SirajiddinUrgench State University, Kh. Alimjan str. 14, Urgench, 221100, UzbekistanFayzullo ShayimovKimyo International University in Tashkent, Shota Rustaveli street 156, Tashkent, 100121, Uzbekistan
Nuclear Physics Bjournal2026en
ABI

Аннотация

In this study, we investigate the attributes of compact stars within the configuration of f ( G , φ ) gravity, by incorporating the Gauss-Bonnet term G and a scalar field φ. By adopting different functional forms of f ( G , φ ) , we analyze their impact on the equilibrium structure of dense stellar objects. Further, we adopt the Krori-Barua metric potential, defined as ν ( r ) = B r 2 + C and λ ( r ) = A r 2 , here, A, B and C are constants. To ensure a physically viable compact configuration, we impose matching conditions between the interior spherically symmetric space-time and the Schwarzschild geometry. Moreover, we investigate the attributes of the celestial star models by assuming the f ( G , φ ) gravity model. We attain the modified field equations and examine key physical characteristics, namely energy density and pressure components, stability conditions, equation of state, and energy constraints. These findings provide new insights into the viability of alternative gravity models in explaining extreme astrophysical environments and offer potential observational signatures to constrain f ( G , φ ) gravity through future gravitational wave and electromagnetic observations.

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