production of light flavor hadrons
play

Production of light flavor hadrons at intermediate and high p T - PowerPoint PPT Presentation

Production of light flavor hadrons at intermediate and high p T measured with ALICE Michael Linus Knichel for the ALICE Collaboration Universitt Heidelberg May 19, 2014 Particle production at intermediate and high p T pp p-Pb Pb-Pb Pb p p


  1. Production of light flavor hadrons at intermediate and high p T measured with ALICE Michael Linus Knichel for the ALICE Collaboration Universität Heidelberg May 19, 2014

  2. Particle production at intermediate and high p T pp p-Pb Pb-Pb Pb p p p Pb Pb • test of pQCD • fragmentation • initial and final state cold functions nuclear matter effects • collective effects • tuning of MC • collective effects? • parton energy loss generators • reference for Pb-Pb • modified • reference for fragmentation? p-Pb and Pb-Pb Eskola et al., JHEP 0904:065,2009 Michael L. Knichel Quark Matter 2014, 19.05.2014 2 .

  3. The ALICE detector EMCAL ITS: - electrons SPD-SDD-SSD - γ , π 0 TPC - trigger (SPD) - tracking - tracking - PID - vertex - PID VZERO HMPID - trigger - PID - multiplicity - centrality TRD: 2.8 < η lab < 5.1 - electron ID -3.7 < η lab < -1.7 - tracking Muon spectrometer TOF ZDC - PID magnet - multiplicity B = 0.5 T - control trigger TPC: full length tracks for | η lab | < 0.8 Michael L. Knichel Quark Matter 2014, 19.05.2014 3 .

  4. p T resolution with ALICE detector • best p T resolution with combined TPC+ITS tracking • currently: σ ( p T )/ p T ~ 10% at p T = 50 GeV/ c (pp, Pb-Pb) • p-Pb: improved reconstruction, expected also for pp and Pb-Pb σ ( p T )/ p T ~ 1% at p T = 1 GeV/ c σ ( p T )/ p T ~ 3% at p T = 50 GeV/ c ALICE Collaboration, arXiv:1402.4476 [nucl-ex] Michael L. Knichel Quark Matter 2014, 19.05.2014 4 .

  5. Charged particles in pp • pp is not simple pQCD • uncertainties of NLO only from scale variations μ = 2 p T , μ = p T /2 • PDF and FF uncertainties not included μ r = μ f = μ f‘ = μ = p T NLO: Sassot, Zurita, Stratmann, Phys.Rev D 82, 074011 (2010) PDF: CTEQ6.6M FF: DSS ALICE Collaboration, Eur.Phys.J.C (2013) 73:2662 • NLO overpredicts the cross section by up to a factor 2 • jet spectra are well described e.g. ALICE, Phys. Lett. B 722(2013) 262-272 � FF too hard at LHC energy Michael L. Knichel Quark Matter 2014, 19.05.2014 5 .

  6. pp reference for p-Pb for R pPb a pp reference spectrum is needed ( √ s = 5.02 TeV) • ratio of pp cross sections NLO scaling: at different energies well • charged particles p T > 5 GeV/ c described by NLO ALICE Collaboration, Eur. Phys. J. C (2013) 73:2662 power law interpolation in √ s: • charged particles p T < 5 GeV/ c • π , K, p Michael L. Knichel Quark Matter 2014, 19.05.2014 6 .

  7. Charged particles in p-Pb • minimum bias trigger • NSD collisions • 2013 data, L int = 50.7 µb -1 • 0.15 < p T < 50 GeV/ c • reduced systematic uncertainties • softer spectrum at backward rapidity (Pb side) • in the ratio of η intervals many systematic uncertainties cancel sign convention: proton goes to y > 0, η cms > 0 ALICE Collaboration, arXiv:1405.2737 [nucl-ex] Michael L. Knichel Quark Matter 2014, 19.05.2014 7 .

  8. R pPb of charged particles nuclear modification factor: (pp reference: η < 0.8) • N coll scaling at high p T • N part scaling at low p T N part scaling • small Cronin-like enhancement at ALICE Collaboration, arXiv:1405.2737 [nucl-ex] intermediate p T · R pPb Ò p T ± ± ± (GeV/ c ) | η cms |<0.3 stat. syst. norm. 10-20 0.995 0.007 0.084 0.06 N part scaling 20-28 0.990 0.031 0.090 0.06 28-50 0.969 0.056 0.090 0.06 ‚ T pPb Ò = ‚ N coll Ò / σ NN ; σ NN = 70 ± 5 mb (interpolation) ⇒ σ tot = 2.1 b; ‚ b Ò = 5.56 fm; ‚ N coll Ò = 6.9 ± 0.6; ‚ T pPb Ò = 0.0983 ± 0.0035 mb -1 Michael L. Knichel Quark Matter 2014, 19.05.2014 8 .

  9. Comparison of R pPb to other measurements • ALICE charged jets R pPb • CMS: consistent with unity up to strong anti-shadowing at large p T p T,jet = 100 GeV/ c – not seen in ALICE data • also pp references are different jet R pPb : M. Connors (poster E-06) R. Haake (poster E-09) • ATLAS (0-90%, p T < 22 GeV/ c ) R pPb in agreement with ALICE Michael L. Knichel Quark Matter 2014, 19.05.2014 9 .

  10. R pPb compared to models ALICE Collaboration, arXiv:1405.2737 [nucl-ex] • NLO with EPS09s nPDF: agrees for p T > ~6 GeV/ c • LO with cold nuclear matter effects: not supported by data • HIJING 2.1: stronger decrease of R pPb with p T not seen in data • none of the models reproduces the Cronin enhancement NLO+EPS09s: Helenius et al., JHEP 1207 (2012) 073 LO+CNM: Kang et al., Phys.Lett. B718 (2012) 482-487 HIJING: Xu et al., Phys.Rev. C86 (2012) 051901 not included in the Figure: CGC predictions are for low p T and agree with the data • (rcBK-MC, Albacete et al. Nucl. Phys. A 897, 2013) EPOS3 with hydro describes R pPb and the spectra (within ~20%) • (K. Werner et al., arXiv:1312.1233) PHSD transport model does not describe the spectra for p T > 2 GeV/ c • (V. P. Konchakovski et al., arXiv:1401.4409) Michael L. Knichel Quark Matter 2014, 19.05.2014 10 .

  11. Particle Identification in ALICE ALICE Collaboration, arXiv:1402.4476 [nucl-ex] ALICE Collaboration, arXiv:1402.4476 [nucl-ex] • remark TPC d E /d x ITS d E /d x ALICE Collaboration, arXiv:1402.4476 [nucl-ex] ALICE Collaboration, arXiv:1402.4476 [nucl-ex] Time-of-flight HMPID Cherenkov Michael L. Knichel Quark Matter 2014, 19.05.2014 11 .

  12. TPC relativistic rise d E /d x • fit of 4 Gaussians ( π , K, p, e) in intervals of η and p T • peak positions and width fixed from identified particles • π , K, p spectra on statistical basis for 3 < p T < 20 GeV/ c ε 2 2 d N E d N N = × × π π π ch from TPC d E /d x η ε dydp p d dp N T T ch ch Michael L. Knichel Quark Matter 2014, 19.05.2014 12 .

  13. Identified hadron spectra in p-Pb collisions p-Pb • multiplicity classes from V0A detector • spectra combined from low- p T and high- p T analysis π K p • harder spectra for higher multiplicities • mass ordering of π , K, p: harder spectra � larger mass Michael L. Knichel Quark Matter 2014, 19.05.2014 13 .

  14. Identified hadron spectra in Pb-Pb collisions Pb-Pb • shape of the spectrum in Pb-Pb differs from pp reference • difference most pronounced in central collisions π K p ALICE Collaboration, arXiv:1401.1250 [nucl-ex] Michael L. Knichel Quark Matter 2014, 19.05.2014 14 .

  15. Identified hadron ratios p-Pb p-Pb • no multiplicity dependence in K/ π • K/ π ratio reaches ~0.55 at high p T K/ π p/ π • enhancement of protons at intermediate p T (2-6 GeV/ c ) • p/ π ratio ~0.1 at high p T • results from low- p T (< 3 GeV/ c ) and high- p T (> 3 GeV/ c ) analysis Michael L. Knichel Quark Matter 2014, 19.05.2014 15 .

  16. Identified hadron ratios in Pb-Pb collisions • p/ π up to ~0.8 around p T = 3 GeV/ c (central 0-5%) Pb-Pb • K/ π and p/ π diferent from pp at intermediate p T (radial flow) • at large p T particle fractions do not differ from those in pp p/ π K/ π ALICE Collaboration, arXiv:1401.1250 [nucl-ex] Michael L. Knichel Quark Matter 2014, 19.05.2014 16 .

  17. Identified hadron R pPb • pp reference from interpolation p-Pb • π , K not different charged particle R pPb π K p • mass ordering in the Cronin-region: π , K, p, Ξ Ξ • notable enhancement for p, Ξ • Cronin peak in charged R pPb from protons • R pPb of π , K, p consistent with unity at large p T strange baryons: D. Alexandre, Wed 9:00 Michael L. Knichel Quark Matter 2014, 19.05.2014 17 .

  18. Identified hadron R AA • mass ordering at intermediate p T Pb-Pb • less suppression of protons at intermediate p T • at large p T (> 8 GeV/ c ) no difference between particle species ALICE Collaboration, arXiv:1401.1250 [nucl-ex] Michael L. Knichel Quark Matter 2014, 19.05.2014 18 .

  19. Summary/Conclusion • no deviation from N coll scaling in high p T p-Pb • at large p T R pPb and R AA universal for hadron species particle ratios not different from pp � vacuum fragmentation • mass ordering at intermediate p T similar in p-Pb and Pb-Pb (flow?) • Cronin enhancement in p-Pb caused by protons • description of R pPb over full p T range remains a challenge for models ALICE, Phys. Lett. B 720 (2013) 52–62 CMS, Phys.Rev.Lett.106:212301,2011 CMS, Eur. Phys. J. C 72 (2012) 1945 CMS, Phys. Lett. B 710 (2012) 256 CMS, Phys. Lett. B 715 (2012) 66 ALICE, arXiv:1405.2737 [nucl-ex] collective effects: C. Andrei, Mon 12:00 Michael L. Knichel Quark Matter 2014, 19.05.2014 19 .

  20. Additional Slides

  21. EPS09 nPDF for Pb nuclei Eskola et al., JHEP 0904:065,2009 Michael L. Knichel Quark Matter 2014, 19.05.2014 21 .

  22. R CP of jets and charged particles • R CP of charged jets similar to R CP of charged hadrons at comparable parton p T ALICE Collaboration, arXiv:1405.1849 [nucl-ex] ALICE Collaboration, Phys.Lett. B720 (2013) 52-62 ATLAS Collaboration, Phys.Lett. B719 (2013) 220-241 CMS Collaboration, Eur.Phys.J. C72 (2012) 1945 Michael L. Knichel Quark Matter 2014, 19.05.2014 22 .

  23. R AA double ratio • partial cancellation of systematic uncertainties ALICE Collaboration, arXiv:1401.1250 [nucl-ex] Michael L. Knichel Quark Matter 2014, 19.05.2014 23 .

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend