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    Constraining Weyl-type f(Q,T) gravity with big bang nucleosynthesis

    Jian Ge1,*, Lei Ming2,3,4,†, Shi-Dong Liang4,‡, Hong-Hao Zhang4,§, and Tiberiu Harko5,6,∥

    • 1School of Physics, Sun Yat-Sen University, Guangzhou 510275, People’s Republic of China
    • 2Key Laboratory of Atomic and Subatomic Structure and Quantum Control (Ministry of Education), Guangdong Basic Research Center of Excellence for Structure and Fundamental Interactons of Matter, School of Physics, South China Normal University, Guangzhou 510006, China
    • 3Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, Guangdong-Hong Kong Joint Laboratory of Quantum Matter, South China Normal University, Guangzhou 510006, China
    • 4School of Physics, Sun Yat-Sen University, Guangzhou 510275, People’s Republic of China
    • 5Department of Physics, Babes-Bolyai University, Kogalniceanu Street, Cluj-Napoca, 400084, Romania
    • 6Astronomical Observatory, 19 Ciresilor Street, Cluj-Napoca 400487, Romania

    • *Contact author: 2672537261@qq.com
    • †Contact author: minglei@scnu.edu.cn
    • ‡Contact author: stslsd@mail.sysu.edu.cn
    • §Contact author: zhh98@mail.sysu.edu.cn
    • ∥Contact author: tiberiu.harko@aira.astro.ro

    Phys. Rev. D 111, 124049 – Published 25 June, 2025

    DOI: https://doi.org/10.1103/vvrp-dtfg

    Abstract

    The Weyl-type modified gravity theory is an extension of the f(Q) and f(Q,T) theories, where T is the trace of the matter energy-momentum tensor, and the scalar nonmetricity Q is represented in its standard Weyl form, which is fully determined by a vector field ωμ. The theory provides a solid explanation of the observational data and the evolution of the late-time Universe, offering a geometric explanation of the dark energy. In this work, we investigate the big bang nucleosynthesis (BBN) constraints on several Weyl-type f(Q,T) gravity models. We analyze in detail three distinct cosmological models, each corresponding to a specific choice of the functional form of f(Q,T). The first model adopts a simple linear additive structure in Q and T, the second model is multiplicative in Q and T, while the third is additive in T and the exponential of Q. For each f(Q,T) model, we consider first the cosmological evolution in the radiation dominated era, and then we determine the constraints on the model parameters from the primordial abundances of the light element, helium-4, deuterium, and lithium-7. The abundances of helium-4 and deuterium agree with theoretical predictions, however, the lithium problem, even slightly alleviated, still persists for the considered Weyl-type f(Q,T) models. Generally, these models satisfy the BBN constraints, and thus they represent viable cosmologies describing the entire dynamical timescale of the evolution of the Universe.

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