A kaon beam is produced as pure at with momentum

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Particle Physics & Quantum Fields · Quantum dynamics and its formulations

Symmetry and Flavour, Ch Neutral kaons: mixing, strangeness oscillation and CP violation

Problem

A kaon beam is produced as pure K0K^0 at t=0t=0 with momentum p=3.50 GeV/cp=3.50\,\mathrm{GeV}/c. Take mK=497.6 MeV/c2m_K=497.6\,\mathrm{MeV}/c^2, τS=0.8954×10−10 s\tau_S=0.8954\times10^{-10}\,\mathrm{s} (cτS=2.68 cmc\tau_S=2.68\,\mathrm{cm}), τL=5.116×10−8 s\tau_L=5.116\times10^{-8}\,\mathrm{s}, and ΔmKτS=0.474\Delta m_K\tau_S=0.474. ((a)) Find the first proper time t∗>0t^*\gt0, in units of τS\tau_S, at which a kaon born as K0K^0 is equally likely to be found as K0K^0 or as Kˉ0\bar K^0, excluding the equality that holds once the KSK_S component has essentially all decayed away, which is not an oscillatory crossing. ((b)) Convert t∗t^* to a laboratory distance for this beam and give the common value of P(K0→K0;t∗)=P(K0→Kˉ0;t∗)P(K^0\to K^0;t^*)=P(K^0\to\bar K^0;t^*). ((c)) A thin slab of matter is placed at this distance. State, with a one-sentence reason, whether the slab adds a coherent KSK_S amplitude to the KSK_S amplitude still present in the beam, and whether the effect responsible is a strong- or a weak-interaction one.

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