In this paper, we address the reduced beauty cross section (σredbb̄(x, Q²)) and the beauty structure function (F₂bb̄(x, Q²)), to study the beauty content of a proton. We calculate σredbb̄ and F₂bb̄ in the kₜ-factorization formalism by using the integral form of the Kimber-Martin-Ryskin and Martin-Ryskin-Watt unintegrated parton distribution function with the angular ordering constraint ($AOC$) and the MMHT2014 PDF set as the input. Recently Guiot and van Hameren demonstrated that the upper limit, Kₘₐₓ, of the transverse-momentum integration performed in the kₜ-factorization formalism should be almost equal to Q, where Q is the hard scale, otherwise it leads to an overestimation of the proton structure function (F₂(x, Q²)). In the present work, we show that kₘₐₓ cannot be equal Q at low and moderate energy region, and also by considering the gluon and quark contributions to the same perturbative order and a physical gauge for the gluon, i. e., A^μ q^_μ=0 in the calculation of F₂bb̄ in the kₜ-factorization formalism, we do not encounter any overestimation of the theoretical predictions due to different choices of Kₘₐₓ>Q. Finally, the resulted σredbb̄ and F₂bb̄ are compared to the experimental data and the theoretical predictions. In general, the extracted σredbb̄ and F₂bb̄ based on the KMR and MRW approaches are in perfect agreement with the experimental data and theoretical predictions at high energies, but at low and moderate energies, the one developed from the KMR approach has better consistency than that of MRW approach.
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Naeimeh Olanj (2024) studied this question.
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