We added further references that noted this already some time ago in the context of relativistic Rankine-Hugoniot equations. We also expanded the discussion of the shock-rarefaction wave solution on page 8, emphasizing that this solution is everywhere consistent with the second law of thermodynamics. *) We added a reference to the book chapter by Bressan on page 4. R3.1) add general references on Riemann problem for hyperbolic equations, and some explanations for choosing the correct physical solution r3.1 is request 1 by referee 3 etc.) and how we address them (marked by *) in the revised manuscript. The following is a list of the points raised by the referees (e.g. We also obtain results for theĮntanglement entropy of regions crossed by shock and rarefaction waves and findīoth of them to closely follow the evolution of the energy density. This is reminiscent of a contactĭiscontinuity in the Riemann problem. In the steady state region, a smooth crossover develops between two Steady state with constant temperature and flow velocity, both of which areĪccurately described by a shock rarefaction wave solution of the Riemann Smooth broadening wave towards the hot bath. Shock and a rarefaction wave: A shock wave moves towards the cold bath, and a The time evolution of the energyĭensity that we obtain holographically is consistent with the combination of a Solutions of ideal and viscous hydrodynamics. To analytic solutions of the corresponding Riemann problem and to numeric Initially join together two thermal baths at different temperatures andĬhemical potentials and compare the subsequent evolution of the combined system We present the first holographic simulations of non-equilibrium steady stateįormation in strongly coupled $\mathcal=4$ SYM theory in 3 1 dimensions. Condensed Matter Physics - Computational.This Submission thread is now published as This is not the latest submitted version.
0 Comments
Leave a Reply. |
AuthorWrite something about yourself. No need to be fancy, just an overview. ArchivesCategories |