Griffiths Introduction to Elementary Particles · Problem 4.26

Bound States — David J. Griffiths

Physics — QFT · gell-mann-nishijima-generalized

Problem

(a) The Gell-Mann–Nishijima formula, equation (4.37), was proposed in the early fifties, which is to say long before the discovery of charm, beauty, or truth. Using the table of quark properties (on page 47), and the quark isospin assignments, equation (4.38), deduce the general formula expressing QQ in terms of AA, I3I_3, SS, CC, BB, and TT. (b) Because uu and dd are the only quarks with nonzero isospin, it should be possible to express I3I_3 in terms of UU (``upness'') and DD (``downness''). What's the formula? Likewise, express AA in terms of the flavor numbers UU, DD, SS, CC, BB, and TT. (c) Putting it all together, obtain the formula for QQ in terms of the flavor numbers (that is, eliminate AA and I3I_3 from your formula in part (a)). This final version represents the cleanest statement of the Gell-Mann–Nishijima formula, in the three-generation quark model.

Related theory

Browse the problem library