1. Поликарпов Сергей, 12 апреля 2012, ИТЭФ Статья принята в Physics Letters B 1 марта 2011

2. Outline LHCb detector Decay trees Data analysis, simulation Results  ф mode  f0 mode  ratio f0 to ф Conclusions

3. Детектор LHCb

4. Decay trees

5. Data analysis  33 1/pb data collected with LHCb detector in 2010  J /ψ →μ+ μ− : opposite sign tracks pT > 500 MeV/c, identified as muons, vertex χ2/ndof < 11, tz = dZ(J/psi)/{Pjp/Mjp} > 0.5 ps | M(μ+ μ− ) – 3096.9 | < 48 MeV for further analysis 549, 000 ± 1100 J /ψ signal events in the entire mass range

6. J/psi -> μ+ μ− Crystal Ball function

7.  χ2( IP[ pi (or K) ] == 0) > 9 (pi and K tracks do not come from PV),  Perfect pi/K separation with RICH,  Opposite-sign di-pion candidates -> sum pT > 900 MeV  Opposite-sign di-kaon candidates -> o sum pT > 1000 MeV, o |M(K+ K-) – M(φ) | <20 MeV  B0s : two pions(+ and -) (or kaons) form vertex with a χ2< 10,  with the J /ψ they form the B0s vertex: χ2/ndof< 5,  Angle between P(this B0s candidate ) and direction to the PV <0.68◦ Data analysis(2)

8. Simulations to find out efficiency The efficiencies of having all four decay tracks in the geometric acceptance and satisfying the trigger, track reconstruction and data selection requirements are:  (1.471 ± 0.024)% for J/ψ f0,requiring the π+ π− invariant mass be within ±500 MeV of 980 MeV,  and (1.454 ± 0.021 )%for J /ψ φ,having the K+ K− invariant mass be within ±20 MeV of the φ mass. [Monte Carlo events generated using PYTHIA [..], and LHCb detector simulation based on GEANT4 [..]. ] The uncertainties of the efficiencies are statistical only.

9. RESULTS

10. Mass (J /ψ K+ K−) (in φ-> K+ K− mode) Gaus + pol1 B0s mass =5366.7 ± 0.4 MeV, width = 7.4 MeV 635± 26 events

11. Mass (J/psi pi+ pi-) signal(gaus) B+→J /ψ K+ (π+) 23 ± 9 B→J /ψ π+π− events B0s →J /ψη + B0s → J /ψφ 111± 14 signal events within ±30 MeV of the B0s mass Mass(pi+ pi-) = ( 980±90) MeV

12. Polarization in f0 mode S(B0s) = 0 S(J/ψ ) = 1 S(f0) = 0 J /ψ rest frame B0s f0 f0 rest frame μ+ μ-μ- θJ/ψ θJ/ψ should be distributed as [1− (cos θJ/ψ)^2)] B0s J/ψ π-π- θf0 θf0 should be distributed uniformly (~const) π+π+

13. Angular distributions of events within ± 30 MeV of the B0s mass and± 90 MeV of the f0 mass after like-sign background subtraction. because of efficiency&background effects [1− a*(cos θJ/ψ)^2)]; a= 0.81± 0.21 (fit result) χ2/ndof = 10.3 / 8 χ2/ndof = 15.9/9, Spin(J /ψ) perpendicular to its momentum and a spin-0 f0 meson.

14. Mass(π+ π−) | Mass(J /ψ π+ π−) = Mass(B0s) ± 30 MeV 265 ± 26 events, including 169(+31−21) f0 (980) events 635 +- 26 φ events taking into account efficiencises

15. Model-independent result {M(pi pi) = (980±90) MeV, here are 111 ± 14 events.}

16. Conclusions The first observation of a new CP-odd eigenstate decay mode of the B0s meson into J /ψ f0(980) has been made Using a fit including two interfering resonances, the f0(980 ) and f0(1370),the ratio to J /ψ φ production is measured as By selecting events within ±90 MeV of 980 MeV the ratio becomes R’ = 0.162 ± 0.022 ± 0.016. The events around the f0(980) mass are large enough in Rate and have small enough backgrounds that they could be used to measure βs without angular analysis.

17. BACKUP SLIDES

18. Crystal Ball

21. Systematic uncertaintaes