A sample of mesons ( ) is reconstructed in a silicon vertex detector

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

Symmetry and Flavour, Ch Heavy flavour: charm and beauty decays and the magnitudes of the CKM elements

Problem

A sample of Bs0B_s^0 mesons (mBs0=5.366 GeVm_{B_s^0} = 5.366\,\mathrm{GeV}) is reconstructed in a silicon vertex detector. The tracks have mean lab-frame momentum ⟨p⟩=45 GeV\langle p\rangle = 45\,\mathrm{GeV}, and an exponential fit to the distribution of production-to-decay vertex separations gives a mean decay length ⟨L⟩=3.77 mm\langle L\rangle = 3.77\,\mathrm{mm}. The measured semileptonic branching fraction is Bsl=10.7\mathcal{B}_{\rm sl} = 10.7 percent. Take the Bs0B_s^0 to decay by the same spectator mechanism as the B0B^0, b→c ℓ νˉb \to c\,\ell\,\bar\nu with the light quarks unaffected, so that Γsl=GF2mb5192π3 f(x) ∣Vcb∣2,x=mc2mb2,\Gamma_{\rm sl} = \frac{G_F^2 m_b^5}{192\pi^3}\,f(x)\,|V_{cb}|^2, \qquad x = \frac{m_c^2}{m_b^2}, with mb=4.8 GeVm_b = 4.8\,\mathrm{GeV}, mc=1.5 GeVm_c = 1.5\,\mathrm{GeV}, and f(x)=0.492f(x) = 0.492 for this mass ratio. Use GF=1.166×10−5 GeV−2G_F = 1.166\times10^{-5}\,\mathrm{GeV^{-2}}, ℏ=6.582×10−25 GeV s\hbar = 6.582\times10^{-25}\,\mathrm{GeV\,s} and ℏc=0.1973 GeV fm\hbar c = 0.1973\,\mathrm{GeV\,fm}. ((a)) Using the relativistic relation between lab decay length and proper time, find the mean proper lifetime τBs0\tau_{B_s^0} implied by these vertex data, in picoseconds. ((b)) Using this lifetime and the measured semileptonic branching fraction, extract ∣Vcb∣|V_{cb}|, and compare it with the value Aλ2≈0.042A\lambda^2 \approx 0.042 that Chapter 10 used.

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