Quark?Gluon Plasma Tomography by Vector Mesons

2001 ◽  
Vol 13 (4) ◽  
pp. 289-295
Author(s):  
L.P. Csernai ◽  
I. Lovas ◽  
Zs. Schram ◽  
Á. Nyíri
2013 ◽  
Vol 910-911 ◽  
pp. 482-485
Author(s):  
Rainer J. Fries ◽  
S. De ◽  
D.K. Srivastava

2013 ◽  
Vol 904-905 ◽  
pp. 569c-572c
Author(s):  
Rainer J. Fries ◽  
Somnath De ◽  
Dinesh K. Srivastava

1992 ◽  
Vol 545 (1-2) ◽  
pp. 259-266 ◽  
Author(s):  
W. Barz ◽  
B.L. Friman ◽  
J. Knoll ◽  
H. Schulz

2001 ◽  
Vol 16 (08) ◽  
pp. 531-540 ◽  
Author(s):  
K. OKANO

Within the closed-time-path formalism of nonequilibrium QCD, we derive a Slavnov–Taylor (ST) identity for the gluon polarization tensor. The ST identity takes the same form in both Coulomb and covariant gauges. Application to quasi-uniform quark–gluon plasma (QGP) near equilibrium or nonequilibrium quasistationary QGP is made.


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