6533b852fe1ef96bd12aa39a
RESEARCH PRODUCT
Search for CP violation in D (+/-) -> (KSK +/-)-K-0 and D-s(+/-) -> K-S(0)pi(+/-) decays
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Nuclear and High Energy PhysicsParticle physicsSDG 16 - Peacemedia_common.quotation_subjectCP violation; Hadron-Hadron ScatteringDalitz plotLHCb - Abteilung HofmannHadrons01 natural sciencesAsymmetryNOSettore FIS/04 - Fisica Nucleare e SubnucleareNuclear physicsTEV PP COLLISIONS; PRODUCTION ASYMMETRY0103 physical sciencesCP violation hadron-hadron scatteringPiTEV PP COLLISIONS010306 general physicsLarge Hadron Collider (France and Switzerland)PRODUCTION ASYMMETRYQCmedia_commonPhysicsLuminosity (scattering theory)Hadron-Hadron Scattering010308 nuclear & particles physicshep-exSDG 16 - Peace Justice and Strong InstitutionsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsParticle physicsPhi meson/dk/atira/pure/sustainabledevelopmentgoals/peace_justice_and_strong_institutionsJustice and Strong InstitutionsCP violationCP violationHigh Energy Physics::ExperimentFísica nuclearFísica de partículesExperimentsParticle Physics - Experimentdescription
A search for \CP violation in Cabibbo-suppressed $D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}$ and $D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}$ decays is performed using $pp$ collision data, corresponding to an integrated luminosity of 3~fb$^{-1}$, recorded by the LHCb experiment. The individual $CP$-violating asymmetries are measured to be \begin{eqnarray*} \mathcal{A}_{CP}^{D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}} & = & (+0.03 \pm 0.17 \pm 0.14) \% \mathcal{A}_{CP}^{D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}} & = & (+0.38 \pm 0.46 \pm 0.17) \%, \end{eqnarray*} assuming that $CP$ violation in the Cabibbo-favoured decays is negligible. A combination of the measured asymmetries for the four decay modes $D^{\pm}_{(s)}\rightarrow K^0_{\mathrm{S}} K^{\pm}$ and $D^{\pm}_{(s)}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}$ gives the sum \[ \mathcal{A}_{CP}^{D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}} + \mathcal{A}_{CP}^{D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}} = (+0.41 \pm 0.49 \pm 0.26) \%. \] In all cases, the first uncertainties are statistical and the second systematic. The results represent the most precise measurements of these asymmetries to date and show no evidence for CP violation.
year | journal | country | edition | language |
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2014-10-03 |