Abstract
The CP asymmetry in B− → Ds−D0 and B− → D−D0 decays is measured using LHCb data corresponding to an integrated luminosity of 3.0 fb−1, collected in pp collisions at centre-of-mass energies of 7 and 8 TeV. The results are {mathcal{A}}^{CP}left({B}^{-}to {D}_s^{-}{D}^0right)=left(-0.4pm 0.5pm 0.5right)%kern0.5em mathrm{and}kern0.5em {mathcal{A}}^{CP}left({B}^{-}to {D}^{-}{D}^0right)=left(2.3pm 2.7pm 0.4right)% , where the first uncertainties are statistical and the second systematic. This is the first measurement of {mathcal{A}}^{CP}left({B}^{-}to {D}_s^{-}{D}^0right) and the most precise determination of {mathcal{A}}^{CP}left({B}^{-}to {D}^{-}{D}^0right) . Neither result shows evidence of CP violation.
Highlights
The determinations of ACP (B− → D(−s)D0) are based on the measurements of the raw asymmetries
The tracking system provides a measurement of momentum, p, of charged particles with a relative uncertainty that varies from 0.5% at low momentum to 1.0% at 200 GeV/c
The decay products from each vertex are constrained to originate from a common vertex, the B− vertex is constrained to originate from the associated primary vertex (PV), and the invariant masses of the D0 and the D(−s) mesons are constrained to their known masses [34], To reduce the combinatorial background, while keeping the signal efficiency as large as possible, a multivariate selection based on a boosted decision tree (BDT) [37, 38] is applied
Summary
Precise measurements of the CP asymmetry in B− → D−D0 decays are from the Belle and BaBar experiments, ACP = (0 ± 8 ± 2)% [16] and ACP = (−13 ± 14 ± 2)% [17], respectively, where the first uncertainties are statistical and the second systematic. The CP asymmetry in B− → Ds−D0 decays has not been measured before. B− → D−D0 decays, using pp collision data corresponding to an integrated luminosity of
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have