Testing radiative energy loss at RHIC and the LHC N. Armesto Fifth International Conference on PERSPECTIVES IN HADRONIC PHYSICS: Particle-Nucleus and Nucleus-Nucleus.

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Presentation transcript:

Testing radiative energy loss at RHIC and the LHC N. Armesto Fifth International Conference on PERSPECTIVES IN HADRONIC PHYSICS: Particle-Nucleus and Nucleus-Nucleus Scattering at Relativistic Energies ICTP, Trieste, May 22nd-26th 2006 Néstor Armesto Departamento de Física de Partículas and Instituto Galego de Física de Altas Enerxías Universidade de Santiago de Compostela 1 See the talks by F. Arleo, N. Bianchi, D. d’Enterria, B. Z. Kopeliovich, H. J. Pirner, J. W. Qiu, C. A. Salgado and U. A. Wiedemann

Contents N. Armesto Testing radiative energy loss at RHIC and the LHC 1. Motivation. 2. Model. 3. Results for RHIC. 4. Results for the LHC. 5. Single electrons at RHIC. 6. Conclusions. 2 With Andrea Dainese (Padova), Carlos A. Salgado and Urs A. Wiedemann (CERN), Phys. Rev. D71 (2005) (hep-ph/ ). With the former plus Matteo Cacciari (Paris VI), hep-ph/ (Phys. Lett. B in press).

1. Motivation (I): (Baier et al '00; Kovner et al '03; Gyulassy et al '03) N. Armesto Testing radiative energy loss at RHIC and the LHC 3 Medium-induced gluon radiation dominant over elastic scattering at high parton E (~ p T at y=0): ● Degrades the energy of the leading hadron: jet quenching. ● Broadens the associated parton shower. ● Increases the associated hadron multiplicity., The BDMPS(-GLV-ZW-WZ) formalism describes this in pQCD: interference of production and re-scatterings of the radiated gluon leading to ➔ Interference and mass effects: Transport coefficient

1. Motivation (II): N. Armesto Testing radiative energy loss at RHIC and the LHC 4 N. Armesto 4 It has become the ‘canonical’ explanation for the suppression of leading particle spectra at large p T and y=0: ➔ Magnitude of the suppression:. ➔ Dependence of the suppression with centrality and azimuth: L 2. ➔ Disappearance of back-to-back correlations: NP, tangential emission? To further test it and constrain parameters: ➔ High p T particle correlations, jet shapes and multiplicities. color charge mass effect Genuine prediction of this approach:  E (g) >  E (q) >  E (Q)

1. Motivation (III): N. Armesto Testing radiative energy loss at RHIC and the LHC 5 N. Armesto 5 ● Heavy-to-light ratios R D,B/h =R AA D,B /R AA h : sensitive to (Armesto et al '05) ➔ Color-charge dependence (g to light hadrons important, increases R D,B/h ). ➔ Mass dependence (Q radiate less, increases R D,B/h ). ● Massive partons radiate less in the vacuum: dead cone effect, postulated for the medium (Dokshitzer-Kharzeev '01). ● Technically: rescattering+dead cone (Djordjevic et al '03; Zhang et al '03; Armesto et al '03). ➔ Detailed behavior of the partonic p T spectrum (softer for Q, increases R D,B/h ) and fragmentation functions (harder for Q, decreases R D,B/h ).

2. Model (I): N. Armesto Testing radiative energy loss at RHIC and the LHC 6 Standard LO pQCD (PYTHIA): Quenching weights ( : probability for medium energy loss, they contain a no-eloss contribution. ➔ CTEQ4L pdf's, EKS98. ➔ All channels into account. ➔ Ff into D (B) and semileptonic e-decays. ➔ RHIC: tune to STAR D-meson data. ➔ LHC: tune to NLO pQCD calculation. RHIC, no medium effects

2. Model (II): N. Armesto Testing radiative energy loss at RHIC and the LHC 7 (Dainese et al '04, '05; Eskola et al '04) p T parton >5 GeV Detailed modeling of geometry. Eskola et al '04 (Quark Matter 05) Dainese, talk at PANIC05 D'Enterria '05 Dainese et al '04  s =1/3-1/2

3. Results for RHIC: N. Armesto Testing radiative energy loss at RHIC and the LHC 8 R D/h =R AA D /R AA h (Dokshitzer-Kharzeev ’01). ➔ q/g difference affects all p T. ➔ Mass effects sizeable for p T <12 GeV. ➔ Look at 7< p T <12 GeV.

4. Results for the LHC: N. Armesto Testing radiative energy loss at RHIC and the LHC 9 Transport coefficient (density) scaled by multiplicity: factor 2.5 to 7 larger at the LHC than at RHIC (Armesto et al '04, Eskola et al '04). Charm Beauty Small difference between massless c and b. 10<p T <20 GeV: charm sensitive to color (g at low x), bottom to mass.

5. Single electrons at RHIC (I): N. Armesto Testing radiative energy loss at RHIC and the LHC 10 ● RHIC data in AuAu: non-photonic electron spectra (measured - cocktail - conversion: PHENIX '06; STAR '05), weak correlation in p T with parent D, and other contributions (B’s) (Djordjevic et al '05; '06; Armesto et al ‘05). ● Heavy flavor: FONLL (Cacciari et al '98; '01; '05) partonic spectra supplemented with radiative eloss via quenching weights plus FONLL fragmentation: * Uncertainties (mass and scale variation). ● DY: PYTHIA tuned to NLO (Gavin et al '95), it may become important for p T > 10 GeV. ● A 10% contribution from DY may influence R AuAu e as much as 0.1.

5. Single electrons at RHIC (II): N. Armesto Testing radiative energy loss at RHIC and the LHC 11 ● pp data underestimated by FONLL (Cacciari et al ’05). ● Suppression in AuAu compatible with c only. ● Variations in qhat ~ uncertainties. ● v 2 compatible with data (PHENIX '05). pp

5. Single electrons at RHIC (III): N. Armesto Testing radiative energy loss at RHIC and the LHC 12 If R AuAu e <0.4 in the range 5<p T <10 GeV: ● Strong interaction of Q with the medium; hadronization inside, elastic scattering? (Djordjevic et al '06, Hees et al 05, Teaney et al '05). ● Larger transport coefficient? (but upper bound to come, hopefully, from correlations (PHENIX '05; STAR '06) ). ● How well do we control the production of heavy flavors at RHIC? CDF '03, 1.96 TeV

Note: elastic scattering N. Armesto Testing radiative energy loss at RHIC and the LHC 13 ● Historically considered << than radiative eloss (Bjorken '82; Gyulassy-Braaten-Thoma '91). ● Mustafa '05; Djordjevic et al '06; Alam et al '06: new interest due to single electron data, idea extended from heavy to light flavors. ● Peigne et al '05: elastic eloss strongly reduced due to finite L. ● Djordjevic '06: effect of finite interaction time (L) negligible. ● Wang '06: elastic and inelastic elosses in the same multiple scattering formalism. For light flavors: Wang '06, talk at BNL: 20 th J/  birthday  E rad /  E el ~ 3.14  s LT ln(EL/11) ~ 22 for E=10 GeV, T=0.2 GeV, L=6 fm,  s =0.3

6. Conclusions: N. Armesto Testing radiative energy loss at RHIC and the LHC 14 ● Heavy flavors constitute an experimentally accessible testing ground for our understanding of radiative energy loss. ● Both at RHIC and at the LHC heavy-to-light ratios offer solid possibilities to check the formalism like those presented here. ● Single electrons in AuAu at RHIC may demand other effects like elastic scattering, hadronization in medium, strong interactions,… BUT experimental data are not inconsistent with radiative eloss. ● Clarification of this issue will demand (at RHIC and at the LHC): * pp/dAu reference to be controlled. * If possible, data for mesons, not only for electrons. Further work needed: energy constraints, consideration of virtualities,…, crucial for associated particle production.

Backup I: quenching weights N. Armesto Testing radiative energy loss at RHIC and the LHC 15 Mass effect smaller for smaller R=qhat L 3 /2, so smaller for smaller lengths.

Backup II: fixed vs. variable L N. Armesto Testing radiative energy loss at RHIC and the LHC 16 ● m c =1.5 GeV, m b =4.75 GeV; no fragmentation. ● qhat=1.2 GeV 2 /fm with fixed L=6 fm reproduce R AA (0-10%) ~0.2 for pions. ● A large fixed length produces a larger effect of the mass on the eloss: mass effect small for small L. To try to understand a disagreement with Djordjevic et al ‘05

Backup III: bottom in FONLL N. Armesto Testing radiative energy loss at RHIC and the LHC 17 Cacciari et al '03; '04 Reasonable description of b production.

Backup IV: further contraints on qhat N. Armesto Testing radiative energy loss at RHIC and the LHC 18 STAR‘ 06 Tangential emission (Dainese '05) ; associated spectra not yet understood.