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Steffen A. BassJet - Medium Correlations #1 Steffen A. Bass Duke University a model for the medium: 3D-RFD jet energy-loss schemes azimuthally dependent.

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Presentation on theme: "Steffen A. BassJet - Medium Correlations #1 Steffen A. Bass Duke University a model for the medium: 3D-RFD jet energy-loss schemes azimuthally dependent."— Presentation transcript:

1 Steffen A. BassJet - Medium Correlations #1 Steffen A. Bass Duke University a model for the medium: 3D-RFD jet energy-loss schemes azimuthally dependent jet energy-loss Comparison of Jet Energy-Loss Schemes in a 3D Hydrodynamic Medium collaborators: J. Ruppert T. Renk G.Y. Qin C. Nonaka A. Majumder C. Gale

2 Steffen A. BassJet - Medium Correlations #2 Exploring QCD Matter at RHIC and LHC initial state pre-equilibrium QGP and hydrodynamic expansion hadronization hadronic phase and freeze-out Lattice-Gauge Theory: rigorous calculation of QCD quantities works in the infinite size / equilibrium limit Experiments: observe the final state + penetrating probes rely on QGP signatures predicted by Theory Phenomenology & Transport Theory: connect QGP state to observables provide link between LGT and data

3 Steffen A. BassJet - Medium Correlations #3 The Medium: 3D Relativistic Fluid Dynamics C. Nonaka & S.A. Bass, Phys. Rev. C75 014902 (2007)

4 Steffen A. BassJet - Medium Correlations #4 Relativistic Fluid Dynamics transport of macroscopic degrees of freedom based on conservation laws:  μ T μν =0  μ j μ =0 for ideal fluid: T μν = ( ε +p) u μ u ν - p g μν and j i μ = ρ i u μ Equation of State needed to close system of PDE’s: p=p(T, ρ i )  connection to Lattice QCD calculation of EoS initial conditions (i.e. thermalized QGP) required for calculation Hydro assumes local thermal equilibrium, vanishing mean free path This particular implementation:  fully 3+1 dimensional, using ( τ,x,y, η ) coordinates  Lagrangian Hydrodynamics  coordinates move with entropy-density & baryon-number currents  trace adiabatic path of each volume element

5 Steffen A. BassJet - Medium Correlations #5 3D-Hydro: Parameters EOS (entropy density)  =0  0 =0.5   =1.5  max =55 GeV/fm 3, n Bmax =0.15 fm -3  0 =0.6 fm/c longitudinal profile: transverse profile: Initial Conditions: Energy Density: Baryon Number Density: Parameters: Initial Flow: v L =  Bjorken’s solution); v T =0 Equation of State: Bag Model + excluded volume 1 st order phase transition (to be replaced by Lattice EoS)

6 Steffen A. BassJet - Medium Correlations #6 3D-Hydro: Comparison to RHIC separate chemical f.o. simulated by rescaling p,K address all data in the soft sector with one consistent calculation b=6.3 fm Nonaka & Bass: PRC75, 014902 (2007) See also Hirano; Kodama et al.

7 Steffen A. BassJet - Medium Correlations #7 Jet-Medium Correlations: Azimuthally Dependent Jet-Quenching Renk, Ruppert, Nonaka & Bass: Phys. Rev. C75 (2007) 031902 Majumder, Nonaka & Bass: Phys. Rev. C76 (2007) 041902 Qin, Ruppert, Turbide, Gale, Nonaka & Bass: Phys. Rev. C76 (2007) 064907

8 Steffen A. BassJet - Medium Correlations #8 Jet-Quenching: Basic Idea partons lose energy and/or fragment differently than in the vacuum: radiative energy loss  transport coefficient q is sensitive to density of (colored) charges hadrons q q leading particle leading particle fragmentation of hard scattered partons into collimated “jets” of hadrons  p+p reactions provide a calibrated probe, well described by pQCD what happens if partons traverse a high energy density colored medium? What is a jet? hadrons q q leading particle suppressed leading particle suppressed qq g L

9 Steffen A. BassJet - Medium Correlations #9 Jet Energy-Loss Schemes Gyulassy, Levai, Vitev (GLV): medium of heavy static scattering centers w/ Yukawa-like potentials parton picks up transverse kicks ~  2 operator formalism that sums order by order in opacity n=L/ g Armesto, Salgado, Wiedemann (ASW): medium of heavy static scattering centers w/ Yukawa-like potentials parton pics up transverse kicks ~  2 path integral over multiple scatterings in the medium Arnold, Moore, Yaffe (AMY): thermalized partonic medium in HTL approx. (T  and g  0) hard parton comes on-shell, receives hits of  ~gT resummation over multiple scatterings and absorptions Higher Twist (HT): few medium assumptions: short color correlation length calculates modification of n-hadron FF due to mult. scattering in medium scattering encoded as HT gluon-gluon field strength: can be expanded twist- by-twist or resummed for multiple scattering

10 Steffen A. BassJet - Medium Correlations #10 The Soft/Hard Disconnect Heavy-ion collisions at RHIC have produced a state of matter which behaves similar to an ideal fluid  (3+1)D Relativistic Fluid Dynamics and hybrid macro+micro models are highly successful in describing the dynamics of bulk QCD matter Jet energy-loss calculations have reached a high level of technical sophistication (BDMPS, GLV, higher twist…), yet they employ only very simple/primitive models for the evolution of the underlying deconfined medium… all conclusions to be drawn from jet energy-loss calculations are necessarily with respect to the nature of the medium assumed in the calculation  need to overcome this disconnect and treat medium and hard probes consistently and at same level of sophistication!

11 Steffen A. BassJet - Medium Correlations #11 Connecting high-p t partons with the dynamics of an expanding QGP color: QGP fluid density symbols: mini-jets Au+Au 200AGeV, b=8 fm transverse plane@midrapidity Fragmentation switched off hydro+jet model Hydro+Jet model T.Hirano. & Y.Nara: Phys.Rev.C66 041901, 2002 T.Hirano. & Y.Nara: Phys.Rev.C66 041901, 2002  take Parton density ρ (x) from full 3D hydrodynamic calculation x y  use GLV 1 st order formula for parton energy loss (M.Gyulassy et al. ’00) 1 st work combining realistic hydro and jet energy-loss good description of single-inclusive spectra and R AA

12 Steffen A. BassJet - Medium Correlations #12 Higher Twist: fix starting value of q; hadronic phase can be taken into account via coefficient c HG : BDMPS/ASW: define local transport coefficient along trajectory  (K as parameter to fix opacity of medium): Energy-Loss Implementation in 3D RFD 3D hydrodynamic evolution provides , T,  and  QGP as function of ( ,x,y,  ) AMY: evolution of jet-momentum distribution is obtained by solving set of coupled rate eqns, with transition rates depending on the coupling constant  s, local temperature T and flow velocity 

13 Steffen A. BassJet - Medium Correlations #13 Jet-Tomography: Medium Dependence BDMPS/ASW jet energy loss calc. medium modeled via: 1.2+1D Hydro (Eskola et al.) 2.parameterized evolution (Renk) 3.3+1D Hydro (Nonaka & Bass)  ± 50% spread in values for K  large systematic error in tomography analysis due to varying medium descriptions  need standard model for medium to gain predictive and discriminative power

14 Steffen A. BassJet - Medium Correlations #14 AMY & BDMPS Discriminative Power of R AA R AA in (semi-)central collisions is well described by all jet energy-loss schemes parameters reflect tuning of medium structure hard-wired into schemes do differing medium assumptions have impact on analysis?  more sophisticated analysis/observables needed! ASWHTAMY K=3.6q 0 =1.5  s =0.33

15 Steffen A. BassJet - Medium Correlations #15 AMY HT & ASW: Azimuthal Spread ratio of in-plane vs. out-plane R AA shows same & can be easily evaluated as function of centrality  investigate temporal & spatial characteristics of energy-loss in different schemes!  study energy-loss as function of reaction plane and centrality: ASW/BDMPS shows a significantly stronger azimuthal dependence of R AA than AMY & HT

16 Steffen A. BassJet - Medium Correlations #16 Jet Quenching: Differential Analysis R AA in reaction plane T AB : initial number of b.c. length integrated density:  L  ~ q-hat R AA backside rise: tangential emission of jets clear anti-correlation between R AA and q-hat near plateau for q-hat for jets originating in back-hemisphere comparison shows near identical trends for HT and AMY  convergence of approaches allows to shift focus from formalism to physics analysis

17 Steffen A. BassJet - Medium Correlations #17 Summary and Outlook Heavy-Ion collisions at RHIC have produced a state of matter which behaves similar to an ideal fluid and can be well described by RFD jet energy-loss has developed into a sophisticated tool to probe the properties of QCD matter produced at RHIC different energy-loss schemes can only be consistently tested and applied to data if the same hydrodynamic evolution is utilized to describe the underlying medium (currently: BDMPS, HT & AMY) azimuthal dependence of jet energy-loss improves constraints on jet- tomography schemes and parameters  convergence of HT and AMY: formalism under control, now can focus on physics analysis  consistent treatment of hard and soft physics crucial for progress! next step:  probe dependence of results on equation of state and initial cond.  incorporate effects of hard probes on medium

18 Steffen A. BassJet - Medium Correlations #18 Virtual Journal on QCD Matter digest of preprints on  hot & dense QCD matter  the QGP  relat. heavy-ion collisions targeted at graduate students & junior postdocs aims to provide a bigger picture, on how individual publications shape the advancement of the field http://qgp.phy.duke.edu/

19 Steffen A. BassJet - Medium Correlations #19 Hot Quarks 2008 - a conference for young scientists - the premier conference for graduate students, postdocs & junior faculty (up to 12 years post Ph.D.) all areas of experimental and theoretical relativistic heavy-ion physics will be covered August 18 -23 2008 Aspen Lodge at Estes Park, Colorado

20 Steffen A. BassJet - Medium Correlations #20 The End

21 Steffen A. BassJet - Medium Correlations #21 Virtual Journal on QCD Matter digest of preprints on  hot & dense QCD matter  the QGP  relativistic heavy-ion collisions targeted at graduate students & junior postdocs aims to provide a bigger picture, on how individual publications shape the advancement of the field http://qgp.phy.duke.edu/

22 Steffen A. BassJet - Medium Correlations #22 Survey of Transport Approaches

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