Griffiths Introduction to Elementary Particles · Problem 1.8

Elementary Particle Dynamics — David J. Griffiths

Physics — QFT · omega-minus-decay-metastability

Problem

(a) Analyze the possible decay modes of the Ω−\Omega^-, just as you did in Problem 1.7 for the Δ\Delta, Σ∗\Sigma^*, and Ξ∗\Xi^*. See the problem? Gell-Mann predicted that the Ω−\Omega^- would be ``metastable'' (i.e., much longer lived than the other members of the decuplet), for precisely this reason. (The Ω−\Omega^- does in fact decay, but by the much slower weak interaction, which does not conserve strangeness.) (b) From the bubble chamber photograph (Fig.\ 1.11), measure the length of the Ω−\Omega^- track, and use this to estimate the lifetime of the Ω−\Omega^-. (Of course, you don't know how fast it was going, but it's a safe bet that the speed was less than the velocity of light; let's say it was going about 0.1c0.1c. Also, you don't know if the reproduction has enlarged or shrunk the scale, but never mind: this is quibbling over factors of 2, or 5, or maybe even 10. The important point is that the lifetime is many orders of magnitude longer than the 10−2310^{-23} sec characteristic of all other members of the decuplet.)

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