Both and are weak decays of a charged meson to a muon and a (massless

PHYSICS · Multi-part · Fermi University Physics · Particle Physics & Quantum Fields · Particles, interactions and experiment · Particles, interactions and experiment

Particle Physics, Ch Decay rates, cross sections and phase space

Problem

Both π+→μ+νμ\pi^+\to\mu^+\nu_\mu and K+→μ+νμK^+\to\mu^+\nu_\mu are weak decays of a charged meson to a muon and a (massless, for this purpose) neutrino, through vertices of the same general type. The measured lifetimes are τπ=2.603×10−8 s\tau_\pi = 2.603\times10^{-8}\,\mathrm{s} (essentially all to μ+νμ\mu^+\nu_\mu) and τK=1.238×10−8 s\tau_K = 1.238\times10^{-8}\,\mathrm{s}, with B(K+→μ+νμ)=63.56%\mathcal{B}(K^+\to\mu^+\nu_\mu) = 63.56\%. Take mπ=139.57 MeV/c2m_\pi = 139.57\,\mathrm{MeV}/c^2, mK=493.68 MeV/c2m_K = 493.68\,\mathrm{MeV}/c^2, mμ=105.66 MeV/c2m_\mu = 105.66\,\mathrm{MeV}/c^2. ((a)) Find the momentum p∗p^* of the muon in each parent's rest frame (the neutrino is taken massless). ((b)) Find the partial width Γ(→μ+νμ)\Gamma(\to\mu^+\nu_\mu) for both the pion and the kaon. ((c)) State whether the ratio of the two p∗p^* values is reflected in the ratio of partial widths, and what this implies about the squared amplitudes ∣M∣2|\mathcal{M}|^2 of the two decays.

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