Energy loss of a heavy quark from asymptotically AdS geometries

By Christopher P. Herzog. 2006

146 citations recorded by the source corpus.

We investigate some universal features of AdS/CFT models of heavy quark energy loss. In addition, as a specific example, we examine quark damping in the spinning D3-brane solution dual to = 4 SU(N) super Yang-Mills at finite temperature and R-charge chemical potential.

Subfields: Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/2f43640ce07223f092890ad7bda0967b693fb80a

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In Nuclear and High Energy Physics

1. V. Hubeny
2. M. Rangamani
3. S. Gubser
4. T. Takayanagi
5. M. Zamaklar
6. R. Myers
7. D. Harlow
8. Kasper Peeters

Citations in the corpus

• Holographic melting and related properties of mesons in a quark-gluon plasma (2006, background): “(5) In the two backgrounds (1) and (4), the DBI actions have the following form, SconDBI = T̂8 gs ∫ dx4 u4 √ f(u) + R3D4 u3 u′2 f(u) , SdeconDBI = T̂8 gs ∫ dx4 u4 √ f(u) + R3D4 u3 u′2 , (6) where from now on we will drop the subscript on f as it is clear from the context which one should be used.”
• A Holographic View on Physics out of Equilibrium (2010, background): “The first steps to understand the energy loss for probes in plasmas holographically were carried out in the seminal papers [87, 88, 89, 90, 91, 92, 93, 94], by considering the dynamics of probe strings as described above.”
• Brownian Motion in AdS/CFT (2008, unknown): “The Boltzmann factor of Hawking radiation gives an additional factor of 1/(e ω − 1) which scales as (14)Although this is a straightforward generalization of [20, 22] and the general formalism has been laid out in [23], it seems to us that this result has not appeared explicitly in the literature.”
• Momentum fluctuations of heavy quarks in the gauge-string duality (2006, methodology): “Subsequent work includes extensions to nonconformal theories [9, 10, 11, 12], non-zero chemical potentials [13, 14, 15, 16, 17, 18], and other deformations of N = 4 gauge theory [19]; studies of directional emission [20, 21] and the relation to the magnetic string tension [22]; and calculations of d”