We construct and investigate an exact spatially homogeneous but anisotropic Bianchi type-V cosmological model in the framework of linear gravity. A perfect-fluid source with matter Lagrangian is considered. The off-diagonal field equation reduces the directional scale factors to a mean scale factor and a single anisotropy function. An exact hybrid expansion law, is adopted, which naturally produces a transition from decelerated to accelerated expansion. Exact expressions are obtained for the Hubble parameter, deceleration parameter, expansion scalar, shear scalar, mean anisotropy parameter, spatial-curvature term, Ricci scalar, statefinder parameters, energy density, pressure and equation-of-state parameter. For some representative theoretical parameters, the transition from deceleration to acceleration occurs at . The anisotropic contribution decreases rapidly and the model dynamically approaches isotropy. The null, weak and dominant energy conditions remain satisfied over the investigated interval, whereas the strong energy condition becomes violated during the late accelerating epoch. The statefinder pair approaches the CDM fixed point asymptotically. The model therefore provides a simple exact framework for studying modified-gravity effects, anisotropy, spatial curvature and late-time accelerated expansion without introducing additional phenomenological fields.
Introduction
The text presents a theoretical cosmological study of the accelerated expansion of the Universe using a modified theory of gravity and an anisotropic Bianchi type-V cosmological model.
Background
The discovery that the Universe is undergoing accelerated expansion was initially supported by observations of distant Type-Ia supernovae and later confirmed by cosmic microwave background radiation, baryon acoustic oscillations, and large-scale structure observations.
The standard ΛCDM model explains this acceleration using the cosmological constant, Λ, which behaves like a fluid with negative pressure. However, ΛCDM faces two major theoretical problems:
The cosmological-constant problem, involving the large discrepancy between observed vacuum energy and theoretical predictions from quantum field theory.
The cosmic-coincidence problem, concerning why matter and dark-energy densities are comparable specifically around the present cosmic epoch.
These problems motivate alternative explanations based on modified theories of gravity, where cosmic acceleration arises from changes to the gravitational sector rather than an independent dark-energy component.
Modified gravity and Bianchi type-V model
The study considers a modified gravity framework in which the gravitational Lagrangian depends on the Ricci scalar and the trace of the energy-momentum tensor. This creates a direct coupling between matter and geometry and can produce effects capable of influencing cosmic expansion.
The authors use a Bianchi type-V spacetime, an anisotropic but spatially homogeneous cosmological model. This geometry is useful because it allows different spatial directions to expand at different rates while containing the open Friedmann–Lemaître–Robertson–Walker model as its isotropic limit.
The model therefore allows the researchers to investigate:
Cosmic acceleration
Anisotropic expansion
Spatial curvature
Matter–geometry coupling
Evolution toward isotropy
Main objective
The primary goal is to construct an exact anisotropic Bianchi type-V cosmological solution within a linear modified-gravity model.
The study assumes:
A perfect-fluid matter source
A linear form of the modified gravitational function
A hybrid scale factor, combining power-law and exponential expansion
The hybrid scale factor is chosen because it can represent a transition from an early decelerating Universe to a late-time accelerating Universe.
Methodology and mathematical development
The authors begin with the Bianchi type-V metric and derive the modified gravitational field equations using the action principle.
They then:
Introduce a linear functional form for the modified-gravity model.
Use a perfect-fluid energy-momentum tensor.
Derive the modified Einstein field equations.
Integrate the directional equations to obtain the individual scale factors.
Introduce the hybrid scale factor.
Derive the directional and mean Hubble parameters.
Obtain expressions for the expansion, anisotropy, and curvature-related quantities.
Some of the resulting integrals are expressed using the lower incomplete gamma function, allowing exact directional scale factors to be obtained.
Physical quantities investigated
The model is used to study several important cosmological parameters, including:
Energy density
Isotropic pressure
Hubble parameter
Expansion scalar
Shear scalar
Anisotropy parameter
Deceleration parameter
Equation-of-state parameter
Spatial-curvature contribution
Statefinder diagnostic parameters
Energy conditions
The study also examines whether the Universe becomes increasingly isotropic at late times by studying the asymptotic behaviour of the shear and anisotropy parameters.
Conclusion
In this work, we have constructed an exact anisotropic Bianchi type-V cosmological model in linear f(R,T) gravity with f(R,T) = R + 2?T, in units where 8?G = c = 1. A perfect-fluid matter source and the hybrid scale factor a(t) = a?t?e?? have been considered. The hybrid scale factor provides a unified description of cosmic evolution, with power-law expansion at early times and exponential expansion at late times. The exact directional scale factors, energy density, and pressure were obtained from the modified field equations. The parameter ? measures the strength of the matter–geometry coupling, while ? and m characterize the anisotropy and the negative spatial-curvature contribution, respectively. The general-relativistic limit is recovered when ? = 0. The deceleration parameter evolves from a positive value at early times to (q=-1) at late times for (0<1). Thus, the model describes a transition from decelerated to accelerated expansion. The energy density decreases with time, the pressure becomes negative, and the equation-of-state parameter approaches -1. Therefore, the model evolves towards a cosmological-constant-like phase.
The numerical plots, obtained for the illustrative parameter values (a?=1), (?=0.5), (?=0.1), (?=0.1), (m=0.1), and (?=0.1), support the analytical results. The average scale factor grows monotonically, whereas the Hubble parameter approaches a constant value at late times. The shear scalar, mean anisotropy parameter, and spatial-curvature contribution decay as the Universe expands. Consequently, the initially anisotropic Bianchi type-V model approaches an isotropic and effectively spatially flat state in the far future.
The statefinder trajectory approaches the ?CDM fixed point (r,s)=(1,0), which indicates that the late-time behaviour of the model is compatible with the standard cosmological scenario. The energy-condition analysis shows that the late-time violation of the strong energy condition is consistent with accelerated cosmic expansion. At the same time, the resulting expressions for the energy density and pressure allow the null, weak, and dominant energy conditions to be tested for different ranges of the model parameters.
Hence, the present model provides a simple exact framework for studying the combined influence of matter–geometry coupling, anisotropy, and negative spatial curvature on the evolution of the Universe. It also shows that a hybrid expansion law in f(R,T) gravity can reproduce a transition to an accelerating and isotropic late-time Universe without introducing an explicit dark-energy fluid. A detailed observational estimation of the model parameters using Type-Ia supernova, Hubble, baryon-acoustic-oscillation, and cosmic-microwave-background data may be considered in future work. Further extensions may include bulk viscosity, anisotropic fluids, time-dependent coupling parameters, or perturbative stability analysis.
References
[1] A. G. Riess et al., “Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant,” The Astronomical Journal 116, 1009–1038 (1998).
[2] S. Perlmutter et al., “Measurements of ? and ? from 42 High-Redshift Supernovae,” The Astrophysical Journal 517, 565–586 (1999).
[3] D. J. Eisenstein et al., “Detection of the Baryon Acoustic Peak in the Large-Scale Correlation Function of SDSS Luminous Red Galaxies,” The Astrophysical Journal 633, 560–574 (2005).
[4] E. Komatsu et al., “Seven-Year Wilkinson Microwave Anisotropy Probe Observations: Cosmological Interpretation,” The Astrophysical Journal Supplement Series 192, 18 (2011).
[5] Planck Collaboration, N. Aghanim et al., “Planck 2018 Results. VI. Cosmological Parameters,” Astronomy & Astrophysics 641, A6 (2020).
[6] S. Weinberg, “The Cosmological Constant Problem,” Reviews of Modern Physics 61, 1–23 (1989).
[7] P. J. Steinhardt, “Cosmological Challenges for the Twenty-First Century,” in Critical Problems in Physics (Princeton University Press, Princeton, 1997), pp. 123–152.
[8] E. J. Copeland, M. Sami, and S. Tsujikawa, “Dynamics of Dark Energy,” International Journal of Modern Physics D 15, 1753–1936 (2006).
[9] S. Nojiri and S. D. Odintsov, “Introduction to Modified Gravity and Gravitational Alternative for Dark Energy,” International Journal of Geometric Methods in Modern Physics 4, 115–146 (2007).
[10] T. P. Sotiriou and V. Faraoni, “f(R) Theories of Gravity,” Reviews of Modern Physics 82, 451–497 (2010).
[11] A. De Felice and S. Tsujikawa, “f(R) Theories,” Living Reviews in Relativity 13, 3 (2010).
[12] T. Harko, F. S. N. Lobo, S. Nojiri, and S. D. Odintsov, “f(R,T) Gravity,” Physical Review D 84, 024020 (2011).
[13] M. Sharif and M. Zubair, “Energy Conditions in f(R,T) Gravity,” Journal of the Physical Society of Japan 82, 014002 (2013).
[14] S. D. Odintsov and D. Sáez-Gómez, “f(R,T) Gravity and Effective Dark Energy,” Physics Letters B 725, 437–444 (2013).
[15] G. F. R. Ellis and M. A. H. MacCallum, “A Class of Homogeneous Cosmological Models,” Communications in Mathematical Physics 12, 108–141 (1969).
[16] M. P. Ryan and L. C. Shepley, Homogeneous Relativistic Cosmologies (Princeton University Press, Princeton, 1975).
[17] G. C. Nath and P. Sahu, \"LRS Bianchi type-V cosmological model with perfect fluid in $f(R, T)$ gravity,\" International Journal of Geometric Methods in Modern Physics 15 (2018) 1850116.
[18] B. P. Brahma and M. Dewri, \"Bulk viscous Bianchi type-V cosmological model in f(R, T) theory of gravity,\" Frontiers in Astronomy and Space Sciences 9 (2022) 831431.
[19] C. R. Mahanta, S. Deka, and M. P. Das, \"Bianchi type V universe with time varying cosmological constant and quadratic equation of state in f(R, T) theory of gravity,\" East European Journal of Physics 4 (2020) 103–112.
[20] R. P. Wankhade et al., \"LRS Bianchi type-I Universe with anisotropic dark energy and special form of deceleration parameter in f(R, T) gravity,\" International Journal of Advanced Astronomy 6 (2018) 12–18.
[21] J. F. Koly, M. N. Hossain, R. I. Seum, and M. S. Ali, \"Bianchi Type V anisotropic cosmological model with a dynamic cosmological constant Lambda(t) along with quadratic deceleration parameter in f(R, T) gravity,\" Astrophysics and Space Science 368 (2023) 72.
[22] S. K. Tripathy, B. Mishra, M. Khlopov, and S. Ray, “Cosmological Models with a Hybrid Scale Factor,” International Journal of Modern Physics D 30, 2150075 (2021).
[23] B. Mishra, S. K. Tripathy, and S. Tarai, “Cosmological Models with a Hybrid Scale Factor in an Extended Gravity Theory,” Modern Physics Letters A 33, 1850056 (2018).