Observation of Large CP Violation in the Neutral B Meson System

Transcription

1 Observation of Large CP Violation in the Neutral B Meson System Presentation for PHY7357 final exam Yefan Tao Phys.Rev.Lett.87:091802,2001

2 Background: In 1973, Kobayashi and Maskawa(KM) proposed quark mixing matrix when only u, d and s quarks were know c, b and t quarks were discovered subsequently CP violation in the neutral K meson was observed In 1981, Sanda, Bigi and Carter pointed out that KM model predicted large CP violation in certain decays of B mesons Discovery of B " B " mixing in 1987

3 CP violating asymmetry in the time-dependent rates for intial B " and B " decays to a common CP eigenstate, f $% A t = Γ B" f $% Γ B " f $% Γ B " f $% + Γ B " f $% = ξ. sin2φ 4 sinδm 7 t Γ B " (B " ) f $% : the decay rate for B " (B " ) to f $% at a proper time t after production ξ. : CP-eigenvalue of f $% Δm 7 : mass difference between the two B " mass eigenstates φ 4 : internal angle, defined as φ 4 = π arg ) >? CA? CD

4

5

6 KEKB accelerator: the world's highest luminosity machine 8 GeV e-, 3.5 GeV e+, E GHI = 10.58, Υ 4S BBR Lorentz boost βγ ~ Luminosity L ~ XY cm >[ s >4 Integrated luminosity ~ 710 fb >4 (771 million BBR pairs) Belle Detector: SVD : three-layer silicon vertex detector CDC : 50-layer central drift chamber ACC : aerogel threshold Cerenkov counters TOF : time-of-flight scintillation counters ECL : CsI(Tl) crystals KLM : KL mesons and to identify muons

7 Flavor tagging one of the B mesons decays at time t^_` to a final state, f^_` the accompanying B mesons decays to f $%, at t $% proper time: Δt = t $% t^_`, CP violation appears in A(Δt) Δt is determined from the displacement in z between the f $% and f^_` decay vertices: Δt = b cd ghg = ib ghg Measurement reconstruction of B " f $% decay determination of the b-flavor of B meson measurement of Δt fit of Δt distribution with a likelihood method

8 reconstruction of B " f $% decay ξ. = 1 for J/ψ K I, ψ(2s)k I, χ G4 K I, η G K I ξ. = +1 for J/ψ K m specially, for B " J/ψ K ", K " K I π ", the final state is mixture of even and odd CP depending on the relative orbital angular momentum of the J/ψ and K ". A fit to angular distribution of all J/ψ K shows the final state is primarily ξ. = +1, with the fraction of ξ. = 1 is 0.19±0.04(stat)±0.04(syst) J/ψ and ψ(2s) and reconstructed via their decays into l o l > (l = μ, e) ψ(2s) is also reconstructed via J/ψ π o π >, χ G4 via J/ψγ η G is reconstructed in K o K > π " and K I K > π o modes Different selection algorithm is applied in each decay channel based on the study of MC simulation

9 Identification of B mesons (ξ. = 1) identify B decays using the energy difference ΔE = E GHI t E GHI uv_h, and beam energy constrained mass M ug = GHI ) [ (p GHI t ) [ (E uv_h m t = ±0.15 MeV

10 Identification of B mesons (ξ. = +1) B " J/ψ K m, signal purity is about 61%

11 Identification of b flavor Leptons, charged pions, and kaons that are not associated with a reconstructed CP eigenstate decay well measured tracks: high momentum leptons from b cl > ν low momentum leptons from c sl o ν charged kaons and lambdas from b c s high momentum pions from decays of B " D > (π o, ρ o, a 4 o, etc) low momentum pions from D > D " π > MC sample data is use to determine a category-dependent variable that indicates the b flavor. q, discrete, +1 when B " - like, -1 when B " - like r, event-by-event flavor-tagging dilution factor, ranges from r=0 (no flavor discrimination) to r=1(unambiguous flavor assignment)

12 CP violation after vertexing we find 560 events with q = +1 flavor tags and 577 events with q = 1 observed Dt distributions for the qξ. = +1(solid points) and qξ. = 1(open points) event samples

13 Determination of sin2φ 4 performing an unbinned maximum-likelihood fit of a CP violating probability density function (pdf) to the observed Δt distributions For all modes other than J/ψ K m, use events in background-dominant regions of ΔE vs M ug to study the background and shows that it is negligibly small. For J/ψ K m, main background is B J/ψX where some final states are CP eigenstates. Using MC simulation to determine the fraction of events with definite CP component in each component. sin2φ 4 = 0.99 ± 0.14(stat) ± 0.06(syst)

14 (a)asymmetries for the combined data sample that are obtained by applying the fit to the events in each Δt bin separately (b)corresponding asymmetry for (cc )K I (ξ. = 1) (c) corresponding asymmetry for J/ψ K m (ξ. = +1) (d) non-cp eigenstates

15 Conclusion there exists large CP violation in the neutral B meson system a zero value for sin sin2φ 4 is ruled out at a level greater than 6σ result is consistent with the higher range of values allowed by the constraints of the KM model as well as with previous measurement

16 Reference: K. Abe et al. Phys. Rev. Lett. 87, M. Kobayashi and T. Maskawa, Prog. Theor. Phys. 49, 652 (1973) H. Quinn and A. I. Sanda, Eur. Phys. J. C 15, 626 (2000) Belle Collaboration, A. Abashian, Phys. Rev. Lett. 86, 2509