A theoretical model based on the D4 Lie Algebra and Hermitian Symmetric Spaces D5 / D4xU(1) and E6 / D5xU(1) allows calculation of ratios of tree-level particle masses (quark masses being constituent masses): Me-neutrino = Mmu-neutrino = Mtau-neutrino = 0 Me = 0.5110 MeV (assumed); Md = Mu = 312.8 MeV; Mmu = 104.8 MeV; Ms = 625 MeV; Mc = 2.09 GeV; Mtau = 1.88 GeV; Mb = 5.63 GeV; Mt = 130 GeV; W+/- mass = 80.326 GeV; Z0 mass = 91.862 GeV; Higgs mass = 145.8 GeV; Higgs VEV = 252.5 GeV; and ratios of force strength constants: (Ggravity)(Mproton)2 = 5 x 10-39 (asssumed); EM fine structure constant = 1/137.03608; Gfermi = (Gweak)(Mproton)2 = 1.02 x 10-5; color force strength = 0.6286 (at 0.245 GeV). With Nonperturbative QCD etc taken into accoun...
We study quark and lepton mass matrices in the $$A_4$$ modular symmetry towards the unification of t...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We use the color-spin and flavor-spin interaction Hamiltonians with SU(3) flavor symmetry breaking t...
By analogy with an effective model of charged-lepton mass matrix that, with the inputs of $m^{exp}_e...
My theoretical model ( which I call the D4-D5-E6-E7-E8 VoDou Physics Model, because it is based on t...
It is shown that if, from the starting point of a universal rank-one mass matrix long favoured by ph...
One of the intriguing achievements of the superstring derived standard-like models in the free fermi...
AbstractWe propose a realistic A4 extension of the Standard Model involving a particular quark–lepto...
We propose a realistic A(4) extension of the Standard Model involving a particular quark-lepton mass...
The masses of the $SU(3)\times SU(6)$ hadrons are calculated in the chiral-invariant phase space (CH...
A shell model approach leads to a simple constituent quark model for hadron structure in which meson...
Using phenomenological formulae, we deduce the masses and flavors of quarks from two elementary quar...
Based on the experimental data and estimations of the charged leptons and quarks masses, a close pow...
International audienceThe quark-meson-coupling (QMC) model self-consistently relates the dynamics of...
In the Standard Model, we will deduce a configuration with five texture zeros for the quark mass mat...
We study quark and lepton mass matrices in the $$A_4$$ modular symmetry towards the unification of t...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We use the color-spin and flavor-spin interaction Hamiltonians with SU(3) flavor symmetry breaking t...
By analogy with an effective model of charged-lepton mass matrix that, with the inputs of $m^{exp}_e...
My theoretical model ( which I call the D4-D5-E6-E7-E8 VoDou Physics Model, because it is based on t...
It is shown that if, from the starting point of a universal rank-one mass matrix long favoured by ph...
One of the intriguing achievements of the superstring derived standard-like models in the free fermi...
AbstractWe propose a realistic A4 extension of the Standard Model involving a particular quark–lepto...
We propose a realistic A(4) extension of the Standard Model involving a particular quark-lepton mass...
The masses of the $SU(3)\times SU(6)$ hadrons are calculated in the chiral-invariant phase space (CH...
A shell model approach leads to a simple constituent quark model for hadron structure in which meson...
Using phenomenological formulae, we deduce the masses and flavors of quarks from two elementary quar...
Based on the experimental data and estimations of the charged leptons and quarks masses, a close pow...
International audienceThe quark-meson-coupling (QMC) model self-consistently relates the dynamics of...
In the Standard Model, we will deduce a configuration with five texture zeros for the quark mass mat...
We study quark and lepton mass matrices in the $$A_4$$ modular symmetry towards the unification of t...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We use the color-spin and flavor-spin interaction Hamiltonians with SU(3) flavor symmetry breaking t...