Abstract

A measurement of the time-integrated CP asymmetry in D0 → KS0KS0 decays is reported. The data correspond to an integrated luminosity of about 2 fb−1 collected in 2015–2016 by the LHCb collaboration in pp collisions at a centre-of-mass energy of 13 TeV. The D0 candidate is required to originate from a D*+ → D0π+ decay, allowing the determination of the flavour of the D0 meson using the pion charge. The D0 → K+K− decay, which has a well measured CP asymmetry, is used as a calibration channel. The CP asymmetryfor D0 → KS0KS0 is measured to beACPD0→KS0KS0=4.3±3.4±1.0%,\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$ {\\mathcal{A}}^{CP}\\left({D}^0\\to {K}_S^0{K}_S^0\\right)=\\left(4.3\\pm 3.4\\pm 1.0\\right)\\%, $$\\end{document}where the first uncertainty is statistical and the second is systematic. This result is combined with the previous LHCb measurement at lower centre-of-mass energies to obtainACPD0→KS0KS0=2.3±2.8±0.9%.\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$ {\\mathcal{A}}^{CP}\\left({D}^0\\to {K}_S^0{K}_S^0\\right)=\\left(2.3\\pm 2.8\\pm 0.9\\right)\\%. $$\\end{document}

Highlights

  • ACP (D0 → KS0 KS0 ) = (4.3 ± 3.4 ± 1.0)%, where the first uncertainty is statistical and the second is systematic

  • A sample of flavour-tagged D0 → KS0KS0 decays is obtained by selecting D∗+ mesons that are produced in the primary interaction, with the subsequent decay D∗+ → D0π+

  • Where ND0 is the measured yield of D∗+ → D0π+, D0 → KS0KS0 decays and ND0 is the measured yield of D∗− → D0π−, D0 → KS0KS0 decays. This observable is related to the CP asymmetry by the expression, valid for small asymmetries, Araw ≈ ACP + Aprod + Adet, (1.3)

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Summary

LHCb detector

The LHCb detector [11, 12] is a single-arm forward spectrometer covering the pseudorapidity range 2 < η < 5, designed for the study of particles containing b or c quarks. 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. Different types of charged hadrons are distinguished using information from two ring-imaging Cherenkov (RICH) detectors. The configuration with the magnetic field pointing upwards (downwards), MagUp (MagDown), bends positively (negatively) charged particles in the horizontal plane towards the centre of the LHC ring. At the hardware trigger stage, events are required to have a muon with high pT or a hadron, photon or electron with high transverse-energy deposit in the calorimeters. The interaction of the generated particles with the detector, and its response, are implemented using the Geant toolkit [18, 19] as described in ref. The interaction of the generated particles with the detector, and its response, are implemented using the Geant toolkit [18, 19] as described in ref. [20]

Event selection
Asymmetry measurement
Systematic uncertainties
Results
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