Classical Electrodynamics · Problem 11.21

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · maximum-kinetic-energy-decay

Problem

If a system of mass MM decays or transforms at rest into a number of particles, the sum of whose masses is less than MM by an amount ΔM\Delta M, (a) show that the maximum kinetic energy of the iith particle (mass mim_i) is (Ti)max=ΔM(1−miM−ΔM2M)(T_i)_{\rm max} = \Delta M\left(1 - \frac{m_i}{M} - \frac{\Delta M}{2M}\right) (b) determine the maximum kinetic energies in MeV and also the ratios to ΔM\Delta M for each of the particles in the following decays or transformations of particles at rest: μ→e+ν+νˉK+→π++π−+π+K±→e±+π0+νK±→μ±+π0+νp+pˉ→2π++2π−+π0p+pˉ→K++K−+3π0\begin{aligned} \mu &\to e + \nu + \bar{\nu}\\ K^+ &\to \pi^+ + \pi^- + \pi^+\\ K^\pm &\to e^\pm + \pi^0 + \nu\\ K^\pm &\to \mu^\pm + \pi^0 + \nu\\ p + \bar{p} &\to 2\pi^+ + 2\pi^- + \pi^0\\ p + \bar{p} &\to K^+ + K^- + 3\pi^0 \end{aligned}

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