Abstract
We argue that, within the realm of gauge-gravity duality, for a large class of systems in a steady-state there exists an effective thermodynamic description. This description comes equipped with an effective temperature and a free energy, but no well-defined notion of entropy. Such systems are described by probe degrees of freedom propagating in a much larger background, e.g. N f number of $$ \mathcal{N}=2 $$ hypermultiplets in $$ \mathcal{N}=4 $$ SU(N c ) super Yang-Mills theory, in the limit N f ≪ N c . The steady-state is induced by exciting an external electric field that couples to the hypermultiplets and drives a constant current. With various stringy examples, we demonstrate that an open string equivalence principle determines an unique effective temperature for all fluctuations in the probe-sector. We further discuss various properties of the corresponding open string metric that determines the effective geometry which the probe degrees of freedom are coupled to. We also comment on the non-Abelian generalization, where the effective temperature depends on the corresponding sector of the fluctuation modes.
Highlights
(LHC) at TeV-scale, or the cold atoms at unitarity at eV-scale
We demonstrate that an open string equivalence principle determines an unique effective temperature for all fluctuations in the probe-sector
Let us offer some comments on the dual gauge theory side:3 adding D7-branes amounts to adding an N = 2 hypermultiplets in the background of N = 4 super Yang-Mills (SYM)
Summary
Let us begin by discussing the prototypical model for AdS/CFT, which is obtained by considering the near-horizon limit of a stack of Nc D3-branes sitting at the tip of a singularity. Let us offer some comments on the dual gauge theory side: adding D7-branes amounts to adding an N = 2 hypermultiplets in the background of N = 4 SYM. Where VR3 represents the volume of the R3.7 the physical meaning of the function a(r) becomes clear: it encodes the response current in the flavour sector, which is sourced by the applied constant electric field. Since there is no charge carrier in this phase, the current is identically zero And this will suffice for our purposes, let us consider the case when the black hole in the bulk geometry disappears, i.e. b = 0. From (2.25), the pragmatic role of the function a(r) becomes clear: if we set a(r) = const, the action vanishes at r∗2 = R2E, which is the location of the pseudo horizon. We will study the fluctuations in the bosonic sector
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