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Using an expanded form of Planck-Bohrs quantization method and phenomenological formulae,} {small we deduce the rest masses and intrinsic quantum numbers (I, S, C, b and Q) of all kinds of the lowest energy quarks and baryons, from only one elementary quark family}$epsilon $ {small with S = C = b = 0. The deduced quantum numbers match those found in experiments. The deduced rest masses are consistent with experimental results. This paper predicts some quarks $text{u}_{C}text{(6073),}$}d$_{S}${small (9613)} {small $text{and d}_{b}text{(9333)}$and baryons $Lambda_{c}^{+}$% (6696), $Lambda_{b}$(9959)and $Lambda $(10239).
Using a three step quantization and phenomenological formulae, we can deduce the rest masses and intrinsic quantum numbers (I, S, C, B and Q) of quarks from only one unflavored elementary quark family $epsilon$ with S = C = B = 0 in the vacuum. Then
Using phenomenological formulae, we deduce the masses and quantum numbers of the quarks from two elementary quarks ($epsilon_{u}$ and $epsilon_{d}$) first. Then using the sum laws and a binding energy formula, in terms of the qqq baryon model and SU(
Using phenomenological formulae, we can deduce the rest masses and intrinsic quantum numbers (I, S, C, B and Q) of quarks, baryons and mesons from only one unflavored elementary quark family. The deduced quantum numbers match experimental results exa
Baryons with one or more heavy quarks have been shown, in the context of a nonrelativistic description, to exhibit mass inequalities under permutations of their quarks, when spin averages are taken. These inequalities sometimes are invalidated when s
We report on our calculation of the pion electromagnetic form factor with two-flavors of dynamical overlap quarks. Gauge configurations are generated using the Iwasaki gauge action on a 16^3 times 32 lattice at the lattice spacing of 0.12fm with sea