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Constraining linear form of f(R,G,T)f(\mathcal{R,G,T}) gravity from astrophysical observations of the Pulsar U1724

Published 22 Nov 2025 in gr-qc, astro-ph.GA, and hep-th | (2511.18017v1)

Abstract: In this work we examine the internal structure of compact stars within an extended gravitational framework described by the function f(R,G,T)f(\mathcal{R},\mathcal{G},\mathcal{T}). Throughout this work, the quantity R\mathcal{R} refers to the curvature scalar formed from the Ricci tensor. The term G\mathcal{G} denotes the Gauss--Bonnet curvature invariant, while T\mathcal{T} corresponds to the trace obtained by contracting the matter energy-momentum tensor. Our analysis is directed toward massive radio pulsars with masses above 1.8M1.8\,M_{\odot}, which provide an exceptional testing ground for gravity under conditions inaccessible to laboratory experiments. Adopting the linear form f(R,G,T)=R+αG+βTf(\mathcal{R},\mathcal{G},\mathcal{T})=\mathcal{R}+α\,\mathcal{G}+β\,\mathcal{T} where αα and ββ are parameters of suitable dimensionality,\footnote{αα has dimensions of [L<sup>2][L<sup>{2}] and ββ carries units of [N<sup>1][N<sup>{-1}].} we obtain an exact analytic solution for static anisotropic stellar matter in hydrostatic equilibrium. This solution allows all physical quantities to be expressed in terms of the dimensionless parameters α<em>1=α/R<sup>2,</sup>β</em>1=β/κ<sup>2 α<em>{1}=α/R<sup>{2},\qquad</sup> β</em>{1}=β/κ<sup>{2} together with the compactness C=2GM/(Rc<sup>2)C=2GM/(Rc<sup>{2}). We constraint the two parameters αα and ββ by matching the model with the mass and radius of pulsar \textit{U1724} requires restricting these parameters to α<em>1=±0.023α<em>{1}=\pm0.023 and β</em>1=±0.001β</em>{1}=\pm0.001, where κ<sup>2=8πG/c<sup>4κ<sup>{2}=8πG/c<sup>{4} is the standard Einstein coupling. The resulting stellar configuration satisfies the causal bound on the radial sound speed, $c_{s}<sup>{2}&lt;c<sup>{2}/3$, distinguishing it from the corresponding behaviour in general relativity.

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