Abstract

Abstract A study of mixing and indirect CP violation in D 0 mesons through the determination of the parameters y CP and A Γ is presented. The parameter y CP is the deviation from unity of the ratio of effective lifetimes measured in D 0 decays to the CP eigenstate K + K − with respect to decays to the Cabibbo favoured mode K −π+. The result measured using data collected by LHCb in 2010, corresponding to an integrated luminosity of 29 pb−1, is y CP = (5.5 ± 6.3stat ± 4.1syst) × 10−3. The parameter A Γ is the asymmetry of effective lifetimes measured in decays of D 0 and $ {\overline D^0} $ mesons to K + K −. The result is A Γ = (−5.9 ± 5.9stat ± 2.1syst) × 10−3. A data-driven technique is used to correct for lifetime-biasing effects.

Highlights

  • A study of mixing and indirect CP violation in D0 mesons through the determination of the parameters yCP and AΓ is presented

  • The parameter yCP is the deviation from unity of the ratio of effective lifetimes measured in D0 decays to the CP eigenstate K+K− with respect to decays to the Cabibbo favoured mode K−π+

  • The parameter AΓ is the asymmetry of effective lifetimes measured in decays of D0 and D0 mesons to K+K−

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Summary

Data selection

LHCb is a precision heavy flavour experiment which exploits the abundance of charm particles produced in collisions at the Large Hadron Collider (LHC). Is a single arm spectrometer at the LHC with a pseudorapidity acceptance of 2 < η < 5 for charged particles. High precision measurements of flight distances are provided by the Vertex Locator (VELO), which consists of two halves with a series of semi-circular silicon microstrip detectors. The VELO measurements, together with momentum information from forward tracking stations and a 4 Tm dipole magnet, lead to decay-time resolutions of the order of one tenth of the D0 lifetime. Two Ring-Imaging Cherenkov (RICH) detectors using three different radiators provide excellent pion-kaon separation over the full momentum range of interest. The detector is completed by hadronic and electromagnetic calorimeters and muon stations. The sample corresponding to an integrated lmumeaisnuorseimtyeonfts29pprebs−e1ntoefdpphecroelliasrieonbsaasted√osn=a7dTaetVa recorded during the LHC run in 2010

Trigger selection
Offline selection
Determination of decay-time acceptance effects
Fitting method
Cross-checks and systematic uncertainties
Evaluation of systematic uncertainties
Summary of systematic uncertainties
Results and conclusion
Full Text
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