[The math symbols of this abstract has been partly transcripted by the cataloguer] Time-dependent CP asymmetries in the decay rates of the singly Cabibbo-suppressed decays D(exponentiation)0 → K(exponentiation)+ K(exponentiation)- and D(exponentiation)0 → π(exponentiation)+ π(exponentiation)- are measured in pp collision data at centre-of-mass energies of 7 and 8TeV collected by the LHCb detector during LHC Run I, corresponding to an integrated luminosity of 3 fb(exponentiation)-1. The strong-interaction decay D(exponentiation)*+ → D(exponentiation)*+ -> D(exponentiation)0 π(exponentiation)+ is used to infer the flavour of the D(exponentiation)0 mesons at production. The asymmetries in effective decay widths between D(exponentiation)0 and (overbar)D(exponentiation)0 decays, sensitive to indirect CP violation, are measured to be A(p-adic integers)Γ (D(exponentiation)0 → K(exponentiation)+ K (exponentiation)-) = (-0.30 ± 0.32 ± 0.10) x 10(exponentiation)-3, A(p-adic integers)Γ (D (exponentiation)0 → π (exponentiation)+ π (exponentiation)-) = ( 0.46 ± 0.58 ± 0.12) x 10¡3, where the first quoted uncertainty is statistical, and the second systematic. These measurements show no evidence of CP violation and improve on the precisiopn of the previuos best measurements by nearly a factor of two.

Measurement of the CP violation parameter Aᴦ in D⁰ → K⁺ K־ and D⁰ → π+π– decays / Marino, Pietro; relatore: Morello, Michael Joseph; Scuola Normale Superiore, 16-May-2017.

Measurement of the CP violation parameter Aᴦ in D⁰ → K⁺ K־ and D⁰ → π+π– decays

Marino, Pietro
2017

Abstract

[The math symbols of this abstract has been partly transcripted by the cataloguer] Time-dependent CP asymmetries in the decay rates of the singly Cabibbo-suppressed decays D(exponentiation)0 → K(exponentiation)+ K(exponentiation)- and D(exponentiation)0 → π(exponentiation)+ π(exponentiation)- are measured in pp collision data at centre-of-mass energies of 7 and 8TeV collected by the LHCb detector during LHC Run I, corresponding to an integrated luminosity of 3 fb(exponentiation)-1. The strong-interaction decay D(exponentiation)*+ → D(exponentiation)*+ -> D(exponentiation)0 π(exponentiation)+ is used to infer the flavour of the D(exponentiation)0 mesons at production. The asymmetries in effective decay widths between D(exponentiation)0 and (overbar)D(exponentiation)0 decays, sensitive to indirect CP violation, are measured to be A(p-adic integers)Γ (D(exponentiation)0 → K(exponentiation)+ K (exponentiation)-) = (-0.30 ± 0.32 ± 0.10) x 10(exponentiation)-3, A(p-adic integers)Γ (D (exponentiation)0 → π (exponentiation)+ π (exponentiation)-) = ( 0.46 ± 0.58 ± 0.12) x 10¡3, where the first quoted uncertainty is statistical, and the second systematic. These measurements show no evidence of CP violation and improve on the precisiopn of the previuos best measurements by nearly a factor of two.
Measurement of the CP violation parameter Aᴦ in D(exponentiation)0 → K(exponentiation)+ K(exponentiation)- and D(exponentiation)0 → π(exponentiation)+ π(exponentiation)- decays
16-mag-2017
FIS/01 FISICA SPERIMENTALE
Fisica
CP asymmetries
CP violations
particle physics
Physics
Scuola Normale Superiore
Morello, Michael Joseph
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11384/85887
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