2015
DOI: 10.1007/jhep01(2015)028
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Complexified boost invariance and holographic heavy ion collisions

Abstract: At strong coupling holographic studies have shown that heavy ion collisions do not obey normal boost invariance. Here we study a modified boost invariance through a complex shift in time, and show that this leads to surprisingly good agreement with numerical holographic computations. When including perturbations the agreement becomes even better, both in the hydrodynamic and the far-from-equilibrium regime. One of the main advantages is an analytic formulation of the stress-energy tensor of the longitudinal dy… Show more

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Cited by 6 publications
(3 citation statements)
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“…projectiles is not boost invariant even when they are infinitely thin. The extent to which this is the case was explored in [24] and, quite remarkably, the results fit well [545] with complex deformations of the purely boost invariant flow introduced in [546].…”
Section: Planar Shocksmentioning
confidence: 58%
“…projectiles is not boost invariant even when they are infinitely thin. The extent to which this is the case was explored in [24] and, quite remarkably, the results fit well [545] with complex deformations of the purely boost invariant flow introduced in [546].…”
Section: Planar Shocksmentioning
confidence: 58%
“…68 Curiously, for the high energy shocks there seems to be a reasonably accurate analytic formulation -at least at small rapidities -by using a complexified boost symmetry, even valid in the far-from-equilibrium regime. 69 At later times the low and high energy collisions behave similarly though; they both thermalize fast (shown in figure 5) and deposit all their energy into the plasma.…”
Section: Colliding Shock Wavesmentioning
confidence: 93%
“…where η 0 = 1 √ 2 3 3/4 , we take N c = 1.8 such that the EOS matches lattice data (e/T 4 ≈ 12) [27,28] and Λ has to be extracted from Fig. 1 numerically as Λ = 0.37 1/3 [29], with = √ L R the center of mass energy density per transverse area of the collision (all quantities depend on x ⊥ ). Eq.…”
Section: Introductionmentioning
confidence: 99%