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Measurement of Direct Photons with the PHENIX Detector at RHIC Richard Petti For the PHENIX Collaboration Department of Physics and Astronomy Stony Brook.

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Presentation on theme: "Measurement of Direct Photons with the PHENIX Detector at RHIC Richard Petti For the PHENIX Collaboration Department of Physics and Astronomy Stony Brook."— Presentation transcript:

1 Measurement of Direct Photons with the PHENIX Detector at RHIC Richard Petti For the PHENIX Collaboration Department of Physics and Astronomy Stony Brook University 4 th International Workshop in HEP in the LHC Era – Chile January 4 th, 2012

2 Outline Introduction to photon production in heavy ion collisions (HIC) Methods of measuring direct photons in PHENIX Recent results Direct photon p T spectrum Direct photon v 2 Theory comparison Outlook and Conclusions Jan.4th 2012 R. Petti for PHENIX 2 Introduction to photon production in heavy ion collisions (HIC) Methods of measuring direct photons in PHENIX Recent results Direct photon p T spectrum Direct photon v 2 Theory comparison Outlook and Conclusions

3 Introduction to HIC – Time Evolution 3 Ions coming at each other Initial collision QGP Hadron gas Jan.4th 2012 R. Petti for PHENIX 1 10 10 7 log t (fm/c) Hadron Decays

4 In non-central collisions Spatial anisotropy → pt anisotropy Distribution of particles in ϕ is measured and Fourier decomposed v 2 is a measure of the elliptic flow strength Elliptic Flow (v 2 ) 4 Mom. Asymmetry elliptic flow Larger pressure gradient in plane Jan.4th 2012 R. Petti for PHENIX Spatial asymmetry eccentricity

5 QGP Thermal radiation Jet Fragmentation Bremsstrahlung Jet conversions Direct Photons in HIC 5 Jan.4th 2012 R. Petti for PHENIX Direct photons = (inclusive photons) – (hadron decay photons) Initial collision QGP Hadron gas High p T probe interactions with medium Hadron Gas Thermal radiation Initial collision Hard scattering of partons (prompt production) Pre-thermalized radiation

6 Direct Photons are a Very Useful Probe in HIC Direct photons can probe the early stages of HICs Do not interact strongly with the medium, so can tell us about: Initial temperature of medium Thermalization time of the medium Pre-thermalization radiation Modification of the fragmentation function in medium … Measurement of direct photon p T spectrum Measurement of direct photon elliptic flow 6 Jan.4th 2012 R. Petti for PHENIX

7 Further Physics Motivation R. Petti for PHENIX 7 Assume that beyond some τ 0 the system is thermalized Ideal hydro evolution Vary τ 0 Main points of the paper v 2 of hadrons insensitive to τ 0 v 2 of thermal photons is sensitive Chatterjee, Srivastava PhysRevC79, 021901,’09 Small τ 0 → larger initial temp. → larger QGP contrib. → smaller v 2 Jan.4th 2012

8 Outline Introduction to photon production in heavy ion collisions (HIC) Methods of measuring direct photons in PHENIX Recent results Direct photon p T spectrum Direct photon v 2 Theory comparison Outlook and Conclusions Jan.4th 2012 R. Petti for PHENIX 8

9 The PHENIX Detector 9 Beam Beam Counter (BBC) Centrality Z vertex Reaction plane Reaction Plane Detector (RxNP) Reaction plane Electromagnetic Calorimeter (EMCal) Photon energy and id Pad Chamber (PC) Veto charged tracks Drift Chamber (DC) Charged tracking Ring Imaging Cherenkov detector (RICH) Electron id Jan.4th 2012 R. Petti for PHENIX

10 Techniques for Photon Measurement R. Petti WWND11 10 3 Techniques Large background from hadron decays makes analysis difficult Measure photons that directly deposit energy into the EMCal Works best at higher momentum Measure virtual photons that internally convert into e + e - pairs Allows a clean low p T measurement Yield of virtual photons is related to real photon production Measure real photons that externally convert in material into e + e - pairs Complementary to virtual photon method

11 Direct Photon p T spectra Measure photons in the EMCal Jan.4th 2012 R. Petti for PHENIX 11 PHENIX, arXiv:1105.412

12 Direct Photon p T Spectra at Low p T Measure low mom. direct photons via virtual photons Agrees well in overlap with high p T measurement See a large enhancement below 3 GeV Exponential in shape Jan.4th 2012 R. Petti for PHENIX 12 Au+Au min. bias √s NN = 200 GeV p+p NLO Vogelsang PRL 104, 132301 (2010) T ave = 221  19 stat  19 syst MeV

13 Measuring Virtual Photons 13 Processes which produce photons can also produce virtual photons Decay into low-mass e + e - pairs The relation between photon and pair production can be written as Measure low mass, high momentum dileptons Correspond to nearly real photons Extrapolate back to zero mass Analyze above π 0 mass to remove 90% of hadron background Jan.4th 2012 R. Petti for PHENIX e+e+ e-e-

14 The Dielectron Spectrum 14 Phys. Lett. B 670, 313 (2009) Jan.4th 2012 R. Petti for PHENIX

15 Compare Mass Distribution to Cocktail 15 Phys. Rev. Lett. 104, 132301 (2010) Jan.4th 2012 R. Petti for PHENIX

16 Extracting the Fraction of Direct Photons 16 Phys. Rev. Lett. 104, 132301 (2010) Fit mass distribution with a two-component function f(m ee ) = (1 – r)f c (m ee ) + rf dir (m ee ) Jan.4th 2012 R. Petti for PHENIX

17 Low Momentum Direct Photons from the Virtual Photon Method R. Petti for PHENIX 17 PHENIX has measured low p T direct photon ratio in various collision systems, showing clear enhancement in A-A No significant enhancement Jan.4th 2012 Note: R γ = r + 1

18 Outline Introduction to photon production in heavy ion collisions (HIC) Methods of measuring direct photons in PHENIX Recent results Direct photon p T spectrum Direct photon v 2 Theory comparison Outlook and Conclusions Jan.4th 2012 R. Petti for PHENIX 18

19 Measuring Direct Photon v 2 19 We want to know whether direct photons flow We need three ingredients to calculate the direct photon v 2 Need the inclusive photon v 2 Need the π 0 v 2 (since most of the inclusive photons are from π 0 decays) Need the fraction of direct photons to decay photons (R γ = N inc /N hadron ) Jan.4th 2012 R. Petti for PHENIX

20 Inclusive photon v 2 Photons measured in the EMCal PID consists of Shower shape cut Charged track veto with PC Significant number of hadrons pass cuts below 6 GeV up to 20% below 2 GeV deposited energy Correct for this with GEANT sim 20 Jan.4th 2012 R. Petti for PHENIX

21 Hadron contamination check Hadron contamination can be significant Check with an external conversion analysis Identify photons via conversion in material to dileptons No hadron contamination Two measurements are consistent Hadron contamination in the real photon (EMCal) measurement well understood 21 Jan.4th 2012 R. Petti for PHENIX

22 π 0 v 2 π 0 → γ + γ Two possible scenarios No direct photons Direct photon v 2 similar to hadrons Calculate v 2 BG (BG includes all hadrons, not just pions) from the measured pion v 2 22 Jan.4th 2012 R. Petti for PHENIX

23 Hadron Decay Photon v 2 Want the hadron decay photon v 2 for R γ calculation About 80% come from π 0 We only measure π 0 v 2 Assume v 2 of other hadrons from KE T scaling v 2 modulation and measured meson ratios input into a MC decay generator This is used to calculate the v 2 of photons from hadron decays 23 Phys.Rev.Lett.98:162301,2007 Jan.4th 2012 R. Petti for PHENIX

24 R γ : Inclusive photon to decay photon ratio Dileptons allow a cleaner measurement at low p T Observe significant contribution of direct photons (~15 - 20%) in MB Working on external conversions for another cross check 24 PHENIX, arXiv:1105.412 Jan.4th 2012 R. Petti for PHENIX

25 Direct photon v 2 We observe a significant direct photon signal An thus observe a significant direct photon v 2 Similar to inclusive photon and π 0 v 2 at low momentum v 2 drops to zero for p T > 5 GeV, where hard processes dominate 25 PHENIX, arXiv:1105.4126 Jan.4th 2012 R. Petti for PHENIX

26 Outline Introduction to photon production in heavy ion collisions (HIC) Methods of measuring direct photons in PHENIX Recent results Direct photon p T spectrum Direct photon v 2 Theory comparison Outlook and Conclusions Jan.4th 2012 R. Petti for PHENIX 26

27 What does it mean? Compare to theory (I) Flow takes time to develop QGP photons have small v 2 Hadron gas thermal photons have large v 2 Does not account for data Is there something wrong with this picture? 27 Jan.4th 2012 R. Petti for PHENIX

28 Theory Comparison (II) 28 0-20% Phys. Rev. C 84, 054906 (2011) H. van Hees, C. Gale, R. Rapp Important features/differences from hydrodynamic expansion Larger equilibrium hadronic rates Hadronic phase includes meson-chemical potentials Hadronic phase lasts longer (smaller T fo and larger T ch ) Elliptic flow builds up faster Thermal radiation dominated by hadronic phase Is the QGP window closed? Jan.4th 2012 R. Petti for PHENIX

29 Theory Comparison (III) Nothing about photon production included in model Assume thermal shape and normalize to data Describes effect of Doppler shift Cylindrical expanding fireball 29 V. Pantuev, arXiv:110 Jan.4th 2012 R. Petti for PHENIX

30 Outline Introduction to photon production in heavy ion collisions (HIC) Methods of measuring direct photons in PHENIX Recent results Direct photon p T spectrum Direct photon v 2 Theory comparison Outlook and Conclusions Jan.4th 2012 R. Petti for PHENIX 30

31 Direct photons at the LHC and future prospects A difficult measurement made even harder ALICE working on it Measuring virtual photons External conversion analysis For the future: Need more precise measurement future quantitative understanding of thermal photons RHIC is a premiere facility to study this Dileptons is the way to go for low momentum direct photons External conversions with a well controlled/understood converter 31 Jan.4th 2012 R. Petti for PHENIX

32 Conclusions Observe direct photon R AA consistent with one Observe an excess of direct photons at low momentum which seems to be thermal in origin Observe a significant fraction of direct photons (~15 - 20% of the inclusive at low momentum) Observe that the inclusive photon v 2 is very similar to the background v 2 at low momentum (below 4 GeV) Observe a large (about 15%) direct photon v 2 Currently unexplained by theory Theory too low Direct photon v 2 at high momentum (above 4 GeV) is consistent with zero, which is consistent with the picture of these direct photons originating from initial hard scattering 32 Jan.4th 2012 R. Petti for PHENIX

33 Backups 33 Jan.4th 2012 R. Petti for PHENIX

34 R AA Jan.4th 2012 R. Petti for PHENIX 34 R AA indicates a medium effect

35 Modification of the Fragmentation Function 35 6.89 ± 0.64 9.49 ±1.37 Look at photon-jet correlation Know momentum of the quark jet from photon jet Observe a difference in FF in Au+Au compared to p+p

36 Dependence on t_0 36 Phys. Rev. C 84, 054906 (2011) H. van Hees, C. Gale, R. Rapp Jan.4th 2012 R. Petti for PHENIX

37 Reaction Plane Resolution 37 Jan.4th 2012 R. Petti for PHENIX

38 Extrapolation to zero mass 38 Jan.4th 2012 R. Petti for PHENIX

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