2019/09/30 by A. Vafaee, Kurosh Javidan, K. Javidan +1
Physics and Astronomy · #Combinatorics #Graph #High-Energy Particle Collisions Research #Particle physics #Particle physics theoretical and experimental studies #Parton #Phenomenology (philosophy) #Physics #Quantum Chromodynamics and Particle Interactions #Quark #Vertex (graph theory) #hep-ph
paper · pdf · doi:10.1142/s0217732320502533
19 pages, 5 figures and 2 Tables
openalex created_date 2019/09/12 · arxiv created 2020/05/02 · openalex publication_date 2020/08/06 · arxiv updated 2020/10/28 · openalex updated_date 2026/08/05
This contribution attempts to determine the [Formula: see text]-quark pole mass [Formula: see text] and [Formula: see text] running mass [Formula: see text] with two different approaches at the next-to-next-to-leading order (NNLO) corrections. At the first approach, we derive a relation between the [Formula: see text]-quark pole mass [Formula: see text] and its [Formula: see text] running mass [Formula: see text] at the NNLO corrections based on the perturbative Quantum Chromo Dynamics (pQCD) predictions. At the second approach, we extract numerical values of the [Formula: see text]-quark pole and [Formula: see text] running masses based on the NNLO phenomenology of H1 and ZEUS Collaborations combined beauty vertex production experimental data. Then we discuss about the compatibility between the pQCD theory results and phenomenology approach in determination of the [Formula: see text]-quark pole and [Formula: see text] running masses at the NNLO corrections. Also, we investigate the role and influence of the [Formula: see text]-quark mass as an extra degree of freedom added to the input parameters of the Standard Model Lagrangian, on the improvement of the uncertainty band of the proton parton distribution functions (PDFs) and particularly on the gluon distribution.