Abstract
We study a simple example of holographic thermalization in a confining field theory: the homogeneous injection of energy in the hard wall model. Working in an amplitude expansion, we find black brane formation for sufficiently fast energy injection and a scattering wave solution for sufficiently slow injection. We comment on our expectations for more sophisticated holographic QCD models.
Highlights
For a translationally invariant setup,3 it was shown that this always results in black brane formation at small amplitude
The starting point of our present paper is that a rich structure of black brane solutions can be found in confining holographic models with the dual field theory living in Minkowski spacetime
We have seen that to leading non-trivial order in the amplitude expansion, for short injection times a black brane is formed, whereas for longer injection times, the shell scatters back and forth between the boundary and the hard wall
Summary
To leading nontrivial order in the amplitude ǫ the black brane horizon radius is given by rh ∼ ǫ2/d/δt To this order, the bulk geometry is given by the AdS-Vaidya metric, which has turned out to be a very useful model for holographic thermalization. The starting point of our present paper is that a rich structure of black brane solutions can be found in confining holographic models with the dual field theory living in Minkowski spacetime (as opposed to a cylinder as for global AdS). The location of the hard wall is proportional to the confinement scale Λ of the boundary theory: r0 ≃ Λ This model only has black branes with event horizon ǫ2/d δt larger than r0
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