In the CPLEAR experiment (Chapter 12)

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Particle Physics & Quantum Fields · Flavour, neutrinos and CP violation

Symmetry and Flavour, Ch B mesons: mixing, time-dependent CP asymmetries and the unitarity triangle

Problem

In the CPLEAR experiment (Chapter 12), a neutral kaon is produced by proton-antiproton annihilation, ppˉ→K+π−Kˉ0p\bar p \to K^+\pi^-\bar K^0 or ppˉ→K−π+K0p\bar p \to K^-\pi^+K^0; the charge of the accompanying charged kaon tells which neutral kaon (strangeness +1+1 or −1-1) was produced, and this instant is t=0t=0 for that kaon. At the Υ(4S)\Upsilon(4S), the two neutral BB mesons are produced together in the antisymmetric L=1L=1 state derived from angular-momentum and Bose-symmetry arguments. ((a)) State what physical process fixes the flavour of the CPLEAR kaon at t=0t=0, and what physical process fixes the flavour of each BB meson at the tagging instant ttagt_{\rm tag} in the Υ(4S)\Upsilon(4S) pair. ((b)) Explain why, unlike the CPLEAR kaon, neither Υ(4S)\Upsilon(4S) BB meson can be assigned a definite flavour at the moment of production, and give the quantum-mechanical reason only one of the pair is B0B^0 (and the other Bˉ0\bar B^0) at every instant before either decays. ((c)) At the Υ(4S)\Upsilon(4S) the tagging instant is not seen directly; it is inferred from the separation of the two decay vertices along the beam. SuperKEKB collides 7.0 GeV7.0\ \mathrm{GeV} electrons head on with 4.0 GeV4.0\ \mathrm{GeV} positrons. Find the invariant mass MM of the collision, the boost βγ\beta\gamma of the Υ(4S)\Upsilon(4S) and the mean vertex separation ⟨Δz⟩\langle\Delta z\rangle, taking cτB0=455 μmc\tau_{B^0}=455\ \mu\mathrm{m}. Compare with the 193 μm193\ \mu\mathrm{m} at KEKB and say what the smaller separation asks of the vertex detector.

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