A kaon is produced at time as a pure

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 is produced at time t=0t=0 as a pure K0K^0. Work in the CP-conserving approximation KS≈K1K_S\approx K_1, KL≈K2K_L\approx K_2 (the admixture parameter ϵ∼2×10−3\epsilon\sim2\times10^{-3} is negligible for this problem), with K1=(K0−Kˉ0)/2K_1=(K^0-\bar K^0)/\sqrt2 and K2=(K0+Kˉ0)/2K_2=(K^0+\bar K^0)/\sqrt2. ((a)) Starting from ∣K0(t)⟩|K^0(t)\rangle written as a superposition of K1K_1 and K2K_2, each evolving with its own mass and width, derive P(K0→K0;t)P(K^0\to K^0;t) and P(K0→Kˉ0;t)P(K^0\to\bar K^0;t) in terms of ΓS\Gamma_S, ΓL\Gamma_L, Γˉ=(ΓS+ΓL)/2\bar\Gamma=(\Gamma_S+\Gamma_L)/2 and Δm=mL−mS\Delta m=m_L-m_S. ((b)) Using τS=0.8954×10−10 s\tau_S=0.8954\times10^{-10}\,\mathrm{s}, τL=5.116×10−8 s\tau_L=5.116\times10^{-8}\,\mathrm{s} and Δm τS=0.474\Delta m\,\tau_S=0.474, evaluate both probabilities at t=20 τSt=20\,\tau_S, and say what the result shows about the strangeness content of a kaon beam that is old compared with τS\tau_S.

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