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Exploring High-Pt Physics with TOF in ALICE: Insights and Future Directions

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28 diapositives · 438 Views · Nov 20, 2014

This presentation discusses the significance of Time-of-Flight (TOF) detectors in high-pT physics, highlighting critical findings from the RHIC results and suggesting future methodologies for studying the interactions between hard-scattered partons and dense color mediums. It examines energy loss mechanisms, jet quenching, and fragmentation modifications using data from the ALICE experiment. The work emphasizes the importance of clear particle identification (PID) and theoretical predictions in furthering our understanding of early-stage hot and dense matter evolution and resonance production in high-energy collisions.

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Transcription de la présentation
  1. High Pt physics with TOF ALICE B.V.Zagreev Bologna - 22.01.2008

  2. Outlook • High Pt physics motivation • Why TOF is relevant detector for this physics? • RHIC results • Conclusion • ITEP group activity

  3. gluon radiation Motivation • Investigation of early stage of hot & dense matter evolution • These partons will first travel through a dense color medium. They are expected to lose energy through collision energy loss and medium induced gluon radiation,“jet quenching”. • The magnitude of the energy loss depends on the gluon density of the medium and on the path length

  4. TOF PID performance • At first glance it is impossible to study high Pt with TOF

  5. Single inclusive hadron distribution vs x Medium effects introduced at parton splitting Hump-backed plateau N. Borghini & U. Wiedemann Hep-ph/0506218 z = phadron/Ejet • Quenching effect: decreases of the particles at high z (low x) & increases of the particles at low z (high x) =ln(EJet/phadron) • Fragmentation strongly modified at phadron~1-5 GeV/c even for the highest energy jets • ALICE should be well dedicated to test this x range (tracking down to 100 MeV/c) • EMCal => improves Ejet determination M.E. - ALICE PWG4 meeting - CERN January 15. 2008 - 3

  6. How to use TOF ALICE for high Pt physics? • We can use high Pt (even not identified) charged particle or photon as a trigger and study accompanying particles! • Fragmentation strongly modified at phadron~1-5 GeV/c even for the highest energy jets • We even don’t need jet reconstructions: instead of z we can use z’ = phadron/Eleading particle (need theoretical predictions!) • Fragmentation distributions should also depend on particle type (need theoretical predictions!) =>we need PID in this (TOF) range • From RHIC data the p/π~1 at high Pt => we can enlarge TOF PID range • Actually we have got additional parameter – leading particle momentum vector and now can measure identified particle with respect to this direction (and reaction plane).

  7. What we know from RHIC? • Usually people distinct three Pt regions: • bulk (Pt < 2 GeV) – seems to be driven by thermal properties of the matter. • high Pt > 6 GeV – measured particle spectra are well described by pQCD calculations (except jet quenching effect ). One can use them as hard trigger. • intermediate region – most interesting effects of hard particles (partons) interactions with media. Different theoretical models (jets + recombination/coalescence mechanism), situation is not clear.

  8. Jet quenching

  9. Enhancement of barion production

  10. Enhancement in strange barion production

  11. Azimuthal correlations

  12. Azimuthal correlations • Lot of theoretical explanations of double away-side peak: deflected jet, large gluon radiation, shock waves (Mach cones), Cerenkov radiation • Long-range Δη correlation on the near-side (ridge): coupling of induced radiation to the longitudinal flow, turbulent color fields, anisotropic plasma, interplay of jet-quenching and strong radial flow… • PID in this range (few GeV) can clarify situation => we have wide field for activity

  13. Resonances • Resonances properties (yields, spectra, width, mass) could be different in medium • The resonances which are unaffected by the hadronic medium have to be used φ – meson is of particular interest because • in case of QGP strong enhancement is expected • small cross section of φ interaction with hadron gas • possible bright effect of double mass peak TOF can identify φ up to Pt=4-5 GeV/c

  14. ΦProduction K+K- and e+e- e+e- K+K- • The leptonic channel yield is a little higher than hadronic channel • More accurate measurement is required to confirm whether there is branch ratio modification

  15. φ – meson angle correlations • Such effects probably are enhanced in jet production, as soon as this is a trigger on early stage of reaction.

  16. φ – meson azimuthal correlations

  17. What should be done? • Fragmentation calculations and measurements • relative to leading particle energy z’ = phadron/Eleading particle or ’=ln(Eleadingparticle/phadron) • for different types of particles (π, K, p, φ…) • Different angular correlations of different types of particles, with respect to jet direction, reaction plane etc. • Estimation of background from underlying events

  18. Conclusion • The jets at intermediate Pt of few GeV have been shown to be significantly modified in the both their particle composition and their angular and fragmentation distributions compare to p+p collisions. • High Pt trigger particle provides additional parameter (direction and momentum of this particle) for such investigations of interactions between hard scattered partons and the medium. • ALICE TOF is the relevant detector for this high Pt physics. • We need both theoretical and experimental researches in this area.

  19. ITEP group activity • Simulation of residual correlations in strange particles femptoscopy with TOF (ALIFEMTO package) (Mikhailov, Stavinsky) • Short living resonances feasibility studies (Kiselev) • Direct (thermal & prompt) photons generator for ALIROOT (Kiselev)

  20. Backup