2006/03/23 by M. D. Scadron, M D Scadron, R. Delbourgo +3
Physics and Astronomy · #Bottom quark #Coupling (piping) #Electroweak interaction #Higgs boson #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #Quantum and Classical Electrodynamics #Quark #Standard Model (mathematical formulation) #Top quark #Weinberg angle #hep-ph
paper · pdf · doi:10.1088/0954-3899/32/5/009
published as J.Phys.G32:735-745,2006 · IOP LaTeX, 12 pages, 1 table; PACS nos. 12.15.-y, 12.40.Vv, 14.65.-q, 13.40.Em; accepted for publication in Journal of Physics G
arxiv created 2006/03/23 · openalex publication_date 2006/04/19 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Constituent quark masses can be determined quite well from experimental data in several ways and one can obtain fairly accurate values for all six m q . The strong quark–meson coupling arises from the quark-level linear σ model, whereas e and sin θ w arise from weak interactions when the heavy M W and M Z are regarded as resonances in analogy with the strong KSFR relation. The Higgs boson mass, tied to null expectation value of charged Higgs components, is found to be around 317 GeV. Finally, the experimental CPV phase angle δ and the three CKM angles Θ c , Θ 2 , Θ 3 are successfully deduced from the six constituent quark masses following Fritzsch's approach.