Heavy quark in an expanding plasma in AdS/CFT
arXiv:0904.1874 · doi:10.1088/1126-6708/2009/06/002
Abstract
Using the Janik-Peschanski dual to a Bjorken flow, a Langevin equation is derived for a heavy quark in an expanding N = 4 supersymmetric Yang-Mills plasma. Such a plasma is characterized by a proper-time dependence of the temperature and corresponds to a system out of equilibrium. The analysis first focuses on a quark at rest in the plasma comoving frame. The case of a quark moving across a longitudinally expanding plasma is then considered. The two-point functions for the random noise acting on such heavy quark probes are computed.
17 pages. v2: references added; improved comments on the Schwinger-Keldysh formalism
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Cited by in corpus (16)
- A holographic view on physics out of equilibrium
- Quantum Fluctuations and the Unruh Effect in Strongly-Coupled Conformal Field Theories
- Holographic Lessons for Quark Dynamics
- The dynamics of quark-gluon plasma and AdS/CFT
- Holographic Brownian Motion and Time Scales in Strongly Coupled Plasmas
- Non-equilibrium physics at a holographic chiral phase transition
- Heavy quark energy loss far from equilibrium in a strongly coupled collision
- Effects of Fluid Velocity Gradients on Heavy Quark Energy Loss
- Early-Time Energy Loss in a Strongly-Coupled SYM Plasma
- Drag and jet quenching of heavy quarks in a strongly coupled N=2* plasma
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- Fermionic Schwinger-Keldysh Propagators from AdS/CFT
- Quantum fluctuations and thermal dissipation in higher derivative gravity
- Holographic drag force in non-conformal plasma
- A random walk with heavy flavours