1. The inсlusive produсtion of the meson resonanсes ρ 0 (770), K * (892), f 0 (980), f 2 (1270) in neutrino- nuсleon interaсtions Polyarush A. Yu. INR RAC Поляруш Александр Юрьевич polyarush@inr.ru

2. Overview The inclusive production of the meson resonances ρ 0 (770), K*(892) ±, f 0 (980), f 2 (1270) in neutrino-nucleon charged current (CC) interactions has been studied with the NOMAD detector exposed to the wide band neutrino beam generated by 450-GeV protons at CERN-SPS. For the first time the f 0 (980) meson is observed in neutrino interactions. The significance of its observation is 5 standard deviations. The presence of f 2 (1270) in the neutrino interactions is reliably established. The average multiplicity of all these resonances is measured as a function of several kinematic variables. The experimental results are compared to the multiplicities obtained from a simulation based on the Lund model. Matrix element of spin density matrix for K ∗ (892) meson have been measured.

3. IHEP PS U-70 3

4. Neutrino flux Neutrino sources : π + -› μ + + ν μ K + -› μ + + ν μ K + -› μ + + ν μ + π ~ 1% = 7.8GeV 4

5. Bubble chamber SKAT Пузырьковая камера СКАТ проектировалась и строилась с 1964г. по 1975г. Облучалась в нейтринном канале ИФВЭ с 1975г. по 1989г. 5

6. Event selection A neutrino event was selected for processing if there was an identified muon at the primary vertex; ˆthere were at least 3 tracks (including muon) at the primary vertex; EνCC > 3GeV; the invariant mass of the hadronic system W was higher than 2 GeV. After cuts we obtain 5792 ν μ CC 6

7. Meson resonance ρ 0 (770) Since the ρ 0 is a resonance decaying into π+π-, its analysis is based on the quantitative determination of the corresponding resonance signal in the invariant mass distribution of π+π- combinations. 7

8. Reflections One can see the contribution from several resonances different from ρ 0 (770) (reflections). The largest contribution is from the ω resonance which decays mainly to 3 pions. Since reflections are situated asymmetrically with respect to the ρ 0 (770) position, experiments where a treatment of reflections was absent or was not correct enough may obtain shifted value of the ρ 0 (770) mass. 8

9. Experimental resolution In order to take into account the increase of the widths of the resonances due to the experimental resolution we estimated the invariant mass resolution function corresponding to the propagation of the errors on the track parameters in data as given by the reconstruction program. ∆Г = 47 МэВ 9

10. В массовом распределении пар одинакового знака резонансов быть не должно. 10

11. 11

12. NOMAD detector 12

13. NOMAD detector 47 drift chambers, 2.7 tons 13

14. Typical ν CC event The main goal of the NOMAD experiment was the search ν μ → ν τ oscillation. ν τ CC interactions identified by using kinematical criteria. This required a very good quality of event reconstruction. 14

15. Neutrino beam WANF CERN Neutrino sources: π + -› μ + + ν μ K + -› μ + + ν μ K + -› μ + + ν μ + π at 1% level ν μ in beam ~93% = 43.8GeV 15

16. NOMAD experiment The present analysis is based on the full sample of data of NOMAD. A neutrino event was selected for processing if the primary vertex is inside the following fiducial volume: |X, Y | < 120cm, 10cm < Z < 390cm; there was an identified muon at the primary vertex with momentum p μ >3GeV/c ˆthe invariant mass of the hadronic system W was higher than 2 GeV; ˆthere were at least 3 tracks (including muon) at the primary vertex; ˆthe event should be measured with reasonable accuracy (ΔEvis/Evis < 30%); _ After cuts we obtain 667252 ν μ CC 15927ν μ CC In this analysis the Monte Carlo (MC) simulation software is based on the LEPTO6.1 - JETSET7.4 -Geant321. 16

17. Raw distribution of the invariant π+π- mass in ν μ CC sample. 17

18. Signal extractoin 18

19. Raw distribution of the invariant mass of (π + π + ), (π - π - ) pairs in ν μ CC sample. 19

20. Reflectoins Reflections are contributions to the π + π - − invariant mass distribution from resonances decaying to π + π - + some other particles or contributions from events where not all the particles of a resonance decay are correctly identified and thus a wrong mass is assigned to them. ω → π + π - π 0 20

21. After reflection subtraction 21

22. After the combinatorial background subtraction 22 f0f0 f2f2

23. 23

24. Masses and widths 24 PDG: NOMAD:

25. Compared to other mesons within its mass region the f 0 (980) has a small total width and a low partial width to γγ. A number of nonstandard interpretations of the f 0 (980) state were suggested: one approach regards the f 0 (980) as four quark bound state [1]. Jaffe had combined f 0 (980), a 0 (980), f 0 (470), K*(700) to form a nonet tetraquark states. 25

26. K + K - molecule states. V.N.Gribov has proposed a theory of confinement in QCD, in which the f 0 (980) plays a special role of a novel vacuum scalar state. F.E. Close et al. noticed that signature of Gribov's vacuum scalar states would be a large yield in low multiplicity events. D. Robson proposed an interpretation of the f 0 (980) as scalar glueball. 26

27. 27 M 2 (π+π−) − distribution from D + → π+π+π− decays. Data of E791 collaboration are shown with error bars, the histogram represent a fit without (a) and with a Breit-Wigner resonance (the σ(485)) Eberhard Klempt and Alexander Zaitsev arXiv:0708.4016v1 (Rhys Rep)

28. Previous neutrino experiments 28 Big European Bubble Chamber (BEBC)

29. Previous experiments ВЕВС WA21 15752 νp CC events ̵ 10452 νp CC events Nρ 0 = 2838 ± 245 ± 340 = 0.180±0.016±0.022 N f 2 = 615±226 = 0.047± 0.017 29

30. Previous experiments 30

31. Previous neutrino experiments All the previous experiments observed an overestimation of the average multiplicities of ρ 0 (770) by the Lund model by 50-70%, while the shapes of the Lund distributions were in agreement with the experimental distributions. 1986. BEBC WA21 1991. 31

32. W 2 distribution W 2 = m 2 +2mν –Q 2 − the hadronic invariant mass squared. ν = E ν - E μ The solid line represents the result of the Lund simulation. The dashed line represent a fitted function a+b×lnW 2 32

33. E ν distribution 33

34. Q 2 distribution 34

35. X F distribution x F = 2p L */W Forward production of ρ 0 (770) and f 2 (1270) is stronger than the backward production. 35

36. Z distribution 36 Z =E ρ /E hadr

37. P T 2 distribution The solid line represents the result of the Lund simulation. The dashed straight line represents the result of the fit by the exponent function. A fit performed in the range p 2 T < 0.5(GeV/c)2gives the following result: b = (5.33 ± 0.19)(GeV/c) −2. p 2 T > 0.5(GeV/c)2 we obtain values: b = (4.12 ± 0.12)(GeV/c) −2. 37

38. Gribov theory verification V.N.Gribov has proposed a new theory of confinement in QCD, in which the f 0 (980) plays a special role of a novel vacuum scalar state. F.E.Close et al. noticed that signature of Gribov's vacuum scalar states would be a large yield in low multiplicity events. 38

39. L. Maiania, et al. arXiv:hep-ph/0606217 R AA - nuclear modification factor 39

40. K * (892) + 40 N K*+ = 26676 ± 1784 ± 1863 = 0.026 ± 0.002 ± 0.002

41. K * (892) + For K ∗ + (892) we present the dependencies of production yields for the same kinematic variables. Matrix element of spin density matrix for K ∗ + (892) meson have been measured ρ 00 = 0.40 ± 0.06(stat) ± 0.03(syst.) Result are in agreement within errors with the ρ 00 = 1/3, which corresponds to no spin alignment for this meson. 41

42. K * (892) + 42

43. K * (892) + 43

44. Conclusion 44

45. We checked the dependence on the hadron jet multiplicity in our W range for f 0 (980) against the predictions of the model of Gribov. We see no evidence of the enhanced f 0 (980) production in low multiplicity events. For K ∗ (892) we present the dependencies of production yields for the same kinematic variables. Matrix element of spin density matrix for K ∗ + (892) meson have been measured ρ 00 = 0.40 ± 0.06(stat) ± 0.03(syst.) Result are in agreement within errors with the ρ 00 = 1/3, which corresponds to no spin alignment for this meson. 45