Resonance and low-mass vector meson production in ALICE

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Presentation transcript:

Resonance and low-mass vector meson production in ALICE A. Badalà – INFN Sezione di Catania for the ALICE collaboration Introduction and ALICE performances Resonances identified by their hadronic decay channel in pp collisions (√sNN= 0.9 and 7 TeV) Resonances identified by their leptonic decay channel in pp collisions (√sNN=2.76 and 7 TeV) Resonance results in Pb-Pb (√sNN =2.76 TeV) Conclusions and Prospects LowX meeting – Paphos (Cyprus) 27 June-1 July 2012 1

Resonances in heavy-ion collisions Resonances have lifetimes of about a few tens fm/c resonance ~ fireball Mass (MeV/c2) Width (MeV/c2) cτ(fm) Decay (770) 770 150.7 1.3 π/ φ(1020) 1019 4.26 46 K K/ Σ(1385)± 1385 33 6 Λ π Ξ(1530)0 1530 9 22 Ξ π t~10 fm/c Resonances may give informations on the nuclear matter dynamics and chiral properties Regeneration and rescattering effectsTimescale chemical-kinetic freeze-out Modification of width, mass and branching ratio Space-time evolution of ultrarelativistic heavy ion collision 2 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Resonances and chiral symmetry To study chiral symmetry restoration in terms of mass shift and width broadening, resonance decays from the early stage of the medium need to be extracted The best probes are resonances reconstructed by their leptonic decay channel since leptons are less likely to rescatter in the hadronic medium. However regenerated resonances from the late hadronic phase feed down into this signal ρ0 π- π+ ρ0 + - π- π+ Hadronic decay channel probes late stages of the collision Leptonic decay channel probes all stages of the collision 3 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Resonances in pp collisions Decay of resonances large fraction of the final-state particles early step in understanding pp collisions at LHC, i.e. opportunity to test QCD in a new energy domain In general, resonance production in pp collisions helps in establishing the underlying event structure and the baseline for heavy-ion collisions constraining QCD-inspired models (PYTHIA, PHOJET,etc…) understanding hadronic production processes strangeness production is accessed via strange resonance production 4 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

ALICE Muon Spectrometer Detector: Size: 16 x 26 meters Weight: 10,000 tons 5

Resonance reconstruction Reconstruction based on primary tracks or particles (cut on DCA) , K, p identified via PID detectors (ITS,TPC,TOF) K(892)0  - + K+ (1020)  K+ + K- S(1385)±  L0 + p± X(1530)0  X- + p+  identified by secondary tracks, with opposite charges, within a fiducial volume, + “V0 topology” K+ K*  identified by three secondary tracks, within a fiducial volume, + “Cascade topology” p- (1020) - 0 6 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Particle identification : Basic identification strategy: fit response function in pT bin TOF  ≈ 90 ps TPC dE/dx ≈5-6% pT range of separation within 3σ (GeV/c) For resonances, V0 and cascade analysis PID by a cut (3-5 ) on the relative difference between: TPC TOF π 0.2 ÷ 0.7 0.5 ÷ 2.0 K 0.3 ÷ 0.6 p 0.5 ÷ 1.0 0.5 ÷ 2.5 TPC signal and Bethe-Bloch function TOF signal and integrated time 7 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Invariant mass signal pp 7 TeV K*(892) 60-155 M MB events (1020) *(1520) *(1385)+ *(1530) 8 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

 @ 0.9 and 7 TeV pp, yield and <pT> φ @ 0.9 TeV : ALICE Collaboration, Eur. Phys. J. C71 (2011), 1594 uncert = √(stat2+syst2) Levy fit √s dN/dy T n 0.9 TeV 0.021 ± 0.005 164 ± 91 4.2 ± 2.5 7 TeV 0.0334 ± 0.0008 286 ± 14 7.0 ± 0.6 A rise in the mean pT with collision energy is observed! ISR ((√s)pp = 62 GeV ) parameterization doesn’t describe pp data at LHC energies, while it describes RHIC pp data dNφ/dy increases proportionally to dNch/dy from 0.9 TeV to 7 TeV Charged multiplicity ALICE Collaboration, Eur. Phys. Journal C 68 (2010), 345 9 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Comparison with MC @ 7 TeV pT ≤ 2 GeV/c: good agreement with PYTHIA D6T pT ≥ 2 GeV/c: good agreement with PHOJET PYTHIA tunes describe better the (1020) than (1385) resonance Yellow band: data systematics 10 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

? / and /K ratio The /K ratio doesn’t increase with energy. The / ratio increases with energy both in heavy-ion and in pp collisions. Will the value at LHC energy confirm this trend? At 200 GeV in pp collisions we observe a saturation. The /K ratio doesn’t increase with energy. Same in all system sizes. 11 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

+anti-/ ratio at 7 TeV HIJING (K=2 GeV/fm) rescale factor Pythia Perugia 2011 is a factor 1.5-5 below data. It underpredicts multistrange baryon yield. Predictions of HIJING/BB with a Strong Color Field modeled by an increased string tension are in agreement with the data. 12 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Low-mass dimuon results 13 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Low mass dimuon spectrum in pp collisions at 7 TeV ALICE coll. Phys. Lett. B 710 (2012) 557 Processes contributing to the dimuon mass spectrum are the light meson (,,,,) decays into muons and the correlated semi-leptonic open charm and beauty decay Fit of the dimuon mass spectrum after background subtraction: ● free parameters of the fit are the normalization of , ,  and open charm ● other processes normalized with ratios between cross sections or branching ratios Blue band: syst. uncertainty from bck. subtraction Red band: Sum of all simulated contributions 14 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

 and  cross section @ 7 TeV ALICE coll. Phys. Lett. B 710 (2012) 557 ALICE coll. Phys. Lett. B 710 (2012) 557 LINT=55.7 nb-1 LINT=55.7 nb-1  values p0= 1.16±0.023GeV/c n=2.7±0.2  values p0= 1.44±0.09 GeV/c n=3.2±0.1  = 0.940 ±0.084(stat.) ±0.076(syst.) mb in 2.5<y<4.0 and 1<pt<5 Gev/c  = 5.28 ±0.54(stat.) ±0.49(syst.) mb in 2.5<y<4.0 and 1<pt<5 Gev/c  overestimated by all models except PYTHIA-Perugia0  is reproduced by PHOJET and ATLAS-CSC and D6T PYTHIA tunes, underestimated by Perugia-0 and 2011 tunes 15 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

 KK and μμ @ 7 TeV ALICE results, μμ Phys. Lett. B710 (2012)557. Slope KK consistent with slope μμ (2.5<y<4.0, 1<pt<5 GeV/c) Difference between forward and mid-central rapidity yield as expected from D6T PYTHIA tune  = 0.940 ±0.084(stat.) ±0.076(syst.) mb in 2.5<y<4.0 and 1<pt<5 Gev/c (LHCb) in ALICE range = 1.07±0.15(stat.+syst.) mb LHCb results, KK (2.44<y<4.06, 0.8<pT<5 GeV/c) Phys. Lett. B703(2011)267. 16 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Comparison @ 2.76 and 7 TeV  =0.587 ±0.070(stat.) ± 0.045 (mb) Blue band: syst. uncertainty from bck. subtraction Red band: Sum of all simulated contributions  =0.587 ±0.070(stat.) ± 0.045 (mb) in 2.5<y<4.0 and 1<pt<4 Gev/c and LINT=17.6 nb-1 PHOJET and PYTHIA with ATLAS-CSC and D6T tunes reproduce  17 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Pb- Pb results 18 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Invariant mass signals Pb-Pb @2.76 TeV Hadronic channel Dimuon channel 2.5<y<4.0 |y|<0.5 |y|<0.5 Combinatorial background estimated by event-mixing 19 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

K* and  mass and width K* No width broadening. Mass shift: the same in pp and Pb-Pb collisionsNo medium effect.  No mass shift or width broadening in Pb-Pb collisions 20 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

K*(892) and (1020) raw spectra in Pb-Pb Corrected spectra will come soon. 21 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Summary pp results Yield and transverse momentum spectrum of ((1020), *(1385)) at mid-rapidity and (782) and (1020) at forward rapidity have been measured in 7 TeV pp collisions and 2.76 and 7 TeV pp collisions, respectively, by their hadronic and leptonic decay channel. In pp collisions /K is indipendent of energy, / saturates at the energy above 200 GeV. Forward-( channel) and mid-rapidity (KK channel)  spectra in 7 TeV pp collisions are in agreement considering the different rapidity range. None of PHOJET and PYTHIA tunes give a full satisfactory description of the spectra at mid-rapidity. In particular they underestimate strange baryon resonances yield. PHOJET and ATLAS-CSC and D6T PYTHIA tunes reproduce  (2.5<y<4.0 , 1<pt<5 Gev/c) in pp collisions at 2.76 and 7 TeV.  at 7 TeV is equal to Perugia-0 PYTHIA value. The +anti-/ ratio at |y|<0.5, not reproduced by Pythia Perugia 2011, is in good agreement with a prediction of HIJING/BB model with a SCF modeled with a string tension of 2 GeV/fm. 22 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Summary PbPb results The widths of K*(892) and (1020) are in agreement with the PDG value including the detector effects. Masses of K* are lower in low pt region for all collision systems. ( no medium effect). Yield of resonances will be soon available. 23 A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

THANKS

Backup slides A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

Processes contributing to the mass spectrum Resonances are simulated with an hadronic cocktail generator. Open charm/beauty simulated via a parametrization of PYTHIA. The pt distribution of ,  and  is described by a power-law function (HERA-B parametrization). The parameter p0 and n were tuned iteratively to the results of the analysis. pt distribution of  from measured distribution via two photon decay channel (ALICE coll.). A. Badalà- LowX meeting – Paphos (Cyprus) 27 June-1 July 2012

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