The Color Glass Condensate to the Strongly Interacting Quark Gluon Plasma: Theoretical Developments

2007 ◽  
Vol 787 (1-4) ◽  
pp. 1-8 ◽  
Author(s):  
Larry McLerran
2013 ◽  
Vol 28 (01) ◽  
pp. 1330001 ◽  
Author(s):  
FRANÇOIS GELIS

We review the color glass condensate effective theory, that describes the gluon content of a high energy hadron or nucleus, in the saturation regime. The emphasis is put on applications to high energy heavy ion collisions. After describing initial state factorization, we discuss the glasma phase, that precedes the formation of an equilibrated quark–gluon plasma. We end this review with a presentation of recent developments in the study of the isotropization and thermalization of the quark–gluon plasma.


2005 ◽  
Vol 757 (1-2) ◽  
pp. 1-27 ◽  
Author(s):  
I. Arsene ◽  
I.G. Bearden ◽  
D. Beavis ◽  
C. Besliu ◽  
B. Budick ◽  
...  

2010 ◽  
Vol 25 (32) ◽  
pp. 5847-5864 ◽  
Author(s):  
LARRY MCLERRAN

This lecture concerns the properties of strongly interacting matter (which is described by Quantum Chromodynamics) at very high energy density. I review the properties of matter at high temperature, discussing the deconfinement phase transition. At high baryon density and low temperature, large Nc arguments are developed which suggest that high baryonic density matter is a third form of matter, Quarkyonic Matter, that is distinct from confined hadronic matter and deconfined matter. I finally discuss the Color Glass Condensate which controls the high energy limit of QCD, and forms the low x part of a hadron wave function. The Glasma is introduced as matter formed by the Color Glass Condensate which eventually thermalizes into a Quark Gluon Plasma.


2006 ◽  
Vol 21 (04) ◽  
pp. 694-698 ◽  
Author(s):  
Larry McLerran

I argue that the physics of the scattering of very high energy strongly interacting particles is controlled by a new, universal form of matter, the Color Glass Condensate. I motivate the existence of this matter and describe some of its properties.


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