Elliptic Flow of Thermal Photons/Dileptons

Nuclear Physics A

Volumn 783, Issue 1-4 SPEC. ISS., 2007, Pages 379-386

  Heinz, U ^a   Chatterjee, R ^b   Frodermann, E ^a   Gale, C ^c   Srivastava, D K ^b  

^a OHIO STATE UNIVERSITY   (United States)

^b VARIABLE ENERGY CYCLOTRON CENTRE   (India)

^c MCGILL UNIVERSITY   (Canada)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 33846424545     PISSN: 03759474     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.nuclphysa.2006.11.090     Document Type: Article

References (21)

1. Heinz U., and Kolb P.F. Nucl. Phys. A 702 (2002) 269
2. Huovinen P. Nucl. Phys. A 761 (2005) 296
3. Hirano T., Heinz U., Kharzeev D., Lacey R., and Nara Y. Phys. Lett. B 636 (2006) 299
4. Lappi T., and Venugopalan R. arXiv:nucl-th/0609021
5. The code can be downloaded from URL. http://nt3.phys.columbia.edu/people/molnard/OSCAR/
6. See also. Kolb P.F., Sollfrank J., and Heinz U. Phys. Rev. C 62 (2000) 054909
7. Kolb P.F., and Rapp R. Phys. Rev. C 67 (2003) 044903
8. Chatterjee R., Frodermann E.S., Heinz U., and Srivastava D.K. Phys. Rev. Lett. 96 (2006) 202302
9. Bass S.A., Müller B., and Srivastava D.K. Phys. Rev. Lett. 93 (2004) 162301
10. Arnold P., Moore G.D., and Yaffe L.G. JHEP 0112 (2001) 009
11. Turbide S., Rapp R., and Gale C. Phys. Rev. C 69 (2004) 014903
12. Kolb P.F., and Heinz U. In: Hwa R.C., and Wang X.-N. (Eds). Quark-Gluon Plasma 3 (2004), World Scientific, Singapore 634. nucl-th/0305084
13. c = 170 MeV is properly taken into account, by assigning all hadrons appropriate T-dependent chemical potentials (see discussion in [5]) and folding these also into the photon emission rates. This was not done in [6]
14. Heinz U. AIP Conf. Proc. 739 (2005) 163
15. Fries R.J., Müller B., and Srivastava D.K. Phys. Rev. Lett. 90 (2003) 132301
16. Fries R.J., Müller B., and Srivastava D.K. Phys. Rev. C 72 (2005) 041902R
17. Turbide S., Gale C., and Fries R.J. Phys. Rev. Lett. 96 (2006) 032303
18. R. Chatterjee, C. Gale, U. Heinz, and D.K. Srivastava, in preparation
19. T ) than shown in Fig. 5, similar to the blue dotted line in Fig. 5 describing the hadronic dileptons. This is due to viscous effects in the hadronic phase which do not allow the φ{symbol} mesons to pick up quite as much radial flow as predicted by the ideal fluid dynamical simulation presented here
20. Adler S.S., et al., PHENIX Collaboration. Phys. Rev. C 72 (2005) 014903
21. T. Hirano, U. Heinz, D. Kharzeev, R. Lacey, and Y. Nara, in preparation