Classical Electrodynamics · Problem 12.11

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · muon-spin-precession

Problem

Consider the precession of the spin of a muon, initially longitudinally polarized, as the muon moves in a circular orbit in a plane perpendicular to a uniform magnetic field B\mathbf{B}. (a) Show that the difference Ω\Omega of the spin precession frequency and the orbital gyration frequency is Ω=eBamμc\Omega = \frac{eBa}{m_\mu c} independent of the muon's energy, where a=(g−2)/2a = (g-2)/2 is the magnetic moment anomaly. (Find equations of motion for the components of spin along the mutually perpendicular directions defined by the particle's velocity, the radius vector from the center of the circle to the particle, and the magnetic field.) (b) For the CERN Muon Storage Ring, the orbit radius is R=2.5R = 2.5 meters and B=17×103B = 17 \times 10^3 gauss. What is the momentum of the muon? What is the time dilatation factor γ\gamma? How many periods of precession T=2π/ΩT = 2\pi/\Omega occur per observed laboratory mean lifetime of the muons? [mμ=105.66m_\mu = 105.66 MeV, τ0=2.2×10−6\tau_0 = 2.2 \times 10^{-6} s, a≈α/2πa \approx \alpha/2\pi]. (c) Express the difference frequency Ω\Omega in units of the orbital rotation frequency and compute how many precessional periods (at the difference frequency) occur per rotation for a 300 MeV muon, a 300 MeV electron, a 5 GeV electron (this last typical of the e+e−e^+e^- storage ring at Cornell).

Related theory

Browse the problem library