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Energy Loss of Heavy Quarks from Asymptotically AdS Geometries
High Energy Physics - Theory · Submitted 19 May 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We investigate some universal features of AdS/CFT models of heavy quark energy loss.
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The abstract, sentence by sentence
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 N=4 SU(N_c) super Yang-Mills at finite temperature and R-charge chemical potential.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate some universal features of AdS/CFT models of heavy quark energy loss. | contribution 0.99 | 0.87 | 0.08 | asserted 0.57 |
| s1 | In addition, as a specific example, we examine quark damping in the spinning D3-brane solution dual to N=4 SU(N_c) super Yang-Mills at finite temperature and R-charge chemical potential. | contribution 0.96 | 0.92 | 0.08 | asserted 0.91 |
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The paper
Original abstract
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 N=4 SU(N_c) super Yang-Mills at finite temperature and R-charge chemical potential.
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References
How the literature uses it
32 arXiv papers cite this in 66 sentences
Papers citing it · 29 sentences without a confident label
Builds on it 4 papers
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In this paper, we describe a family of solutions, which interpolate between the equatorial strings of Ref. [ref] and the uplifted strings of Ref. [ref] .
Spinning Dragging Strings · Introduction and Summary · 0.90
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([ref]) with $z_*$ replaced by $z_WH$ is the result for any asymptotically AdS geometry with a horizon [ref] .
Hall Conductivity of Flavor Fields from AdS/CFT · The Drag Force · 0.81
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It is easy to generalize their computation to AdS$_d$ with general $d$, the result being[Although this is a straightforward generalization of [ref] and the general formalism has been laid out in [ref] , it seems to us that this result has not appeared explicitly in the literature.] [equation] In the non-relativistic limit, $v≪1$, this means that the friction constant is [equation] If we use the Sutherland–Einstein relation [ref],[Note that, as explained around [ref], the relation [ref] does not depend on $d$.] we obtain the diffusion constant [equation] which agrees with [ref] for $d=3$.
Brownian motion in AdS/CFT · Brownian motion of the boundary endpoint · 1.00
Uses its method or tool 5 papers
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To calculate the drag force, one should consider a stretching string from the flavor brane and using prescription in [ref] find energy loss at zero and finite temperature cases.
Drag force in asymptotically Lifshitz spacetimes · Introduction · 0.99
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Since the metric components are $t$ independent, the above action may be treated as a one dimensional mechanical system whose momentum is the constant of motion -g_ttg_xx x'/√(-( g_ttg_rr+g_ttg_xx x'^2+g_xxg_rrv^2)) =c=-2πα' π_x=constant, which can be solved for $x'$ leading to [equation] In terms of the constant $π_x$ one has [ref] dE/dt=π_xv , dP/dt=π_x.
Non-relativistic CFT and Semi-classical Strings · Open string and drag force · 0.84
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[ref] , we employ the relativistic relation $|p⃗| = γM v$ with $γ= 1/√(1-v^2)$, and find
Hall Conductivity of Flavor Fields from AdS/CFT · The Drag Force · 0.95
Compares with it 7 papers
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However, Ref. [ref] finds the friction coefficient $μ$ is velocity independent while the corresponding $μ$ of Ref. [ref] is velocity dependent.
Spinning Dragging Strings · Introduction and Summary · 0.95
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See Refs. [ref] for the relation between the strings with and without inflow.] [equation] where $v$ is the velocity of the quark and $r_ws$ is the solution to $α(r_ws)-v^2 γ(r_ws)=0$.
Holographic Brownian Motion and Time Scales in Strongly Coupled Plasmas · Friction coefficient · 0.93
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Similar to the results of [ref] we find the behaviour is determined completely by the physics near the black hole horizon.
A semi-classical recipe for wobbly limp noodles in partonic soup · Introduction · 0.93
Cites it as background 14 papers
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There has been the $AdS/CFT$ calculation of jet quenching parameter [ref] and the drag coefficient which describes the energy loss for heavy quarks in $𝒩=4$ supersymmetric Yang-Mills theory [ref] .
Charge effect and finite 't Hooft coupling correction on drag force and Jet Quenching Parameter · Introduction · 0.93
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We will use this system, widely studied within the holography literature [ref] , to compute the non-linear corrections to the quark dynamics.
Nonlinear Langevin dynamics via holography · Introduction · 0.92
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On the other hand, the study of the physics of trailing strings in the AdS spacetime explained the dissipative and diffusive physics of a quark moving through a field theory plasma, such as the diffusion coefficient and transverse momentum broadening [ref] .
Holographic Brownian Motion and Time Scales in Strongly Coupled Plasmas · Introduction · 0.87
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