Abstract

Measurements of charm mixing parameters from the decay-time-dependent ratio of D0->K+pi- to D0->K-pi+ rates and the charge-conjugate ratio are reported. The analysis uses data, corresponding to 3 fb^{-1} of integrated luminosity, from proton-proton collisions at 7 and 8 TeV center-of-mass energies recorded by the LHCb experiment. In the limit of charge-parity (CP) symmetry, the mixing parameters are determined to be x'^2=(5.5 +- 4.9)x10^{-5}, y'= (4.8 +- 1.0)x10^{-3}, and R_D=(3.568 +- 0.066)x10^{-3}. Allowing for CP violation, the mixing parameters are determined separately for D0 and D0bar mesons yielding A_D = (-0.7 +- 1.9)%, for the direct CP-violating asymmetry, and 0.75 < |q/p|< 1.24 at the 68.3% confidence level, where q and p are parameters that describe the mass eigenstates of the neutral charm mesons in terms of the flavor eigenstates. This is the most precise determination of these parameters from a single experiment and shows no evidence for CP violation.

Highlights

  • Mass eigenstates of neutral charm mesons are linear combinations of flavor eigenstates jD1;2i1⁄4pjD0iÆqjD" 0i, where p and q are complex parameters

  • If CP symmetry is violated, the oscillation rates for mesons produced as D0 and D" 0 can differ, further enriching the phenomenology

  • The study of CP violation in D0 oscillation may lead to an improved understanding of possible dynamics beyond the standard model [4,5,6,7]

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Summary

RD þ

Where t is the decay time, is the average D0 lifetime, and RD is the ratio of suppressed-to-favored decay rates. A WS candidate is discarded if resulting from a D0 candidate that, associated with another pion, forms a RS candidate with MðD0þs Þ within 3 MeV=c2 of the known DÃþ mass This removes about 15% of the WS background with negligible signal loss. The two subsamples contribute approximately equal signal yields with similar purities They require separate treatment due to their differing kinematic distributions and trigger-induced biases. These are corrected for the relative efficiencies for reconstructing KÀþ and KþÀ final states

No CPV
Findings
Xrþi i
Full Text
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