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[PENDING] approach to equilibrium in high energy heavy ion collisions

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Figure 3.12: τP T and τP L as a function of the proper time. µ is related to the saturation scale Q s through Q s = µg 2 .
Figure 3.13: The longitudinal pressure as a function of proper-time for a system initialized with rapidity dependent fluctuations.
Figure 4.3: The quantum evolution is only accessible with other resummation techniques (e.g.
Figure 5.3: Numerical evaluation of the integral defined in eq. (5.31). The line denotes an exponential fit to the envelope.
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