-
1
-
-
33746893788
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.97.052301
-
S.S. Adler (PHENIX Collaboration), Phys. Rev. Lett. 97, 052301 (2006). PRLTAO 0031-9007 10.1103/PhysRevLett.97.052301
-
(2006)
Phys. Rev. Lett.
, vol.97
, pp. 052301
-
-
Adler, S.S.1
-
2
-
-
28844459491
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.95.152301
-
J. Adams (STAR Collaboration), Phys. Rev. Lett. 95, 152301 (2005). PRLTAO 0031-9007 10.1103/PhysRevLett.95.152301
-
(2005)
Phys. Rev. Lett.
, vol.95
, pp. 152301
-
-
Adams, J.1
-
4
-
-
34247892230
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.75.106003
-
J.J. Friess, S.S. Gubser, G. Michalogiorgakis, and S.S. Pufu, Phys. Rev. D 75, 106003 (2007). PRVDAQ 0556-2821 10.1103/PhysRevD.75.106003
-
(2007)
Phys. Rev. D
, vol.75
, pp. 106003
-
-
Friess, J.J.1
Gubser, S.S.2
Michalogiorgakis, G.3
Pufu, S.S.4
-
5
-
-
34347380389
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.75.105023
-
A. Yarom, Phys. Rev. D 75, 105023 (2007). PRVDAQ 0556-2821 10.1103/PhysRevD.75.105023
-
(2007)
Phys. Rev. D
, vol.75
, pp. 105023
-
-
Yarom, A.1
-
6
-
-
34347398649
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.75.125010
-
A. Yarom, Phys. Rev. D 75, 125010 (2007). PRVDAQ 0556-2821 10.1103/PhysRevD.75.125010
-
(2007)
Phys. Rev. D
, vol.75
, pp. 125010
-
-
Yarom, A.1
-
8
-
-
35148889008
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.99.152001
-
P.M. Chesler and L.G. Yaffe, Phys. Rev. Lett. 99, 152001 (2007). PRLTAO 0031-9007 10.1103/PhysRevLett.99.152001
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 152001
-
-
Chesler, P.M.1
Yaffe, L.G.2
-
9
-
-
35748975401
-
-
NUPBBO 0550-3213 10.1016/j.nuclphysb.2007.08.015
-
S.S. Gubser and S.S. Pufu, Nucl. Phys. NUPBBO 0550-3213 B790, 42 (2008). 10.1016/j.nuclphysb.2007.08.015
-
(2008)
Nucl. Phys.
, vol.790
, pp. 42
-
-
Gubser, S.S.1
Pufu, S.S.2
-
10
-
-
33748777108
-
-
JHEPFG 1029-8479 10.1088/1126-6708/2006/07/013
-
C.P. Herzog, A. Karch, P. Kovtun, C. Kozcaz, and L.G. Yaffe, J. High Energy Phys. JHEPFG 1029-8479 07 (2006) 013. 10.1088/1126-6708/2006/07/013
-
J. High Energy Phys.
, vol.2006
, Issue.7
, pp. 013
-
-
Herzog, C.P.1
Karch, A.2
Kovtun, P.3
Kozcaz, C.4
Yaffe, L.G.5
-
11
-
-
33845449477
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.74.126005
-
S.S. Gubser, Phys. Rev. D 74, 126005 (2006). PRVDAQ 0556-2821 10.1103/PhysRevD.74.126005
-
(2006)
Phys. Rev. D
, vol.74
, pp. 126005
-
-
Gubser, S.S.1
-
12
-
-
33750587061
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.97.182301
-
H. Liu, K. Rajagopal, and U.A. Wiedemann, Phys. Rev. Lett. 97, 182301 (2006). PRLTAO 0031-9007 10.1103/PhysRevLett.97.182301
-
(2006)
Phys. Rev. Lett.
, vol.97
, pp. 182301
-
-
Liu, H.1
Rajagopal, K.2
Wiedemann, U.A.3
-
13
-
-
14044254117
-
-
NUPABL 0375-9474 10.1016/j.nuclphysa.2004.12.074
-
H. Stoecker, Nucl. Phys. A750, 121 (2005). NUPABL 0375-9474 10.1016/j.nuclphysa.2004.12.074
-
(2005)
Nucl. Phys.
, vol.750
, pp. 121
-
-
Stoecker, H.1
-
16
-
-
33846889745
-
-
PYLBAJ 0370-2693 10.1016/j.physletb.2007.01.008
-
T. Renk and J. Ruppert, Phys. Lett. B 646, 19 (2007). PYLBAJ 0370-2693 10.1016/j.physletb.2007.01.008
-
(2007)
Phys. Lett. B
, vol.646
, pp. 19
-
-
Renk, T.1
Ruppert, J.2
-
17
-
-
40749101672
-
-
Alternatively, one could associate E and the longitudinal component of the Poynting vector S→•K^ with the sound mode, and the transverse part of S→ (orthogonal to K^) with the diffusion mode. We thank
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Alternatively, one could associate E and the longitudinal component of the Poynting vector S→•K^ with the sound mode, and the transverse part of S→ (orthogonal to K^) with the diffusion mode. We thank D. Teaney for discussions related to these points.
-
-
-
Teaney, D.1
-
18
-
-
40749084798
-
-
http://physics.princeton.edu/~ssgubser/papers/fourier/details.pdf.
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