{"arxiv_id":"hep-th/0607233","incoming":{"papers":18,"sentences":38,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0801.1117","title":"Velocity Dependence of Baryon Screening in a Hot Strongly Coupled Plasma","url":"/paper/0801.1117","section":"Wind parallel to the baryon configuration","sentence":"For example, following a line of reasoning developed in Ref. [ref] for the meson sector, it can be shown that in a certain class of gauge theories whose gravity duals are asymptotically AdS, as $v→1$ the baryon screening length scales as $L_s ∝(1-v^2)^1/4/^1/4$, where $$ is the energy density of the plasma. $$ is proportional to $T^4$ for the specific theory that we have analyzed, at any $v$, in this Section.","intent_p":0.95,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0706.0086","title":"Screening length and the direction of plasma winds","url":"/paper/0706.0086","section":"Introduction","sentence":"In the next section, we briefly summarize our procedure to derive the screening length developed in Ref. [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1106.5008","title":"On non-relativistic $Q\\bar Q$ potential via Wilson loop in Galilean space-time","url":"/paper/1106.5008","section":"$QQ̅$ potential in non-relativistic CFT with Galilean symmetry","sentence":"[ref] , in obtaining the action ([ref]) as well as the corresponding $QQ̅$ potential as a function of $QQ̅$ pair's distance.","intent_p":0.96,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0706.0086","title":"Screening length and the direction of plasma winds","url":"/paper/0706.0086","section":"Setup","sentence":"exponent summarizes the exponent $ν$ for various theories obtained in Ref. [ref] .","intent_p":0.92,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":3,"sentences":3,"quotes":[{"arxiv_id":"0706.0086","title":"Screening length and the direction of plasma winds","url":"/paper/0706.0086","section":"Behavior near $θ= π/2$","sentence":"For the D$p$-brane, L_max-pi_half-lambda_half indeed reduces to our previous result when $θ=π/2$ (Eq. (5.14) of Ref. [ref] ) using $ν=(5-p)/(2(7-p))$ from exponent.","intent_p":0.82,"contests_p":null},{"arxiv_id":"0803.2481","title":"Jet evolution in the N=4 SYM plasma at strong coupling","url":"/paper/0803.2481","section":"Relation with previous approaches","sentence":"In this subsection, we shall show that our previous results are consistent with, and shed new light on, previous studies in the literature [ref] , concerning the propagation of `heavy quarks', or of quark–antiquark `mesons', in the strongly coupled $𝒩=4$ SYM plasma.","intent_p":0.93,"contests_p":null},{"arxiv_id":"0906.2964","title":"Holographic model with a NS-NS field","url":"/paper/0906.2964","section":"Meson in non-commutative QGP","sentence":"If the coordinate $ρ$ is constant, and $ω=0$, then it reduces to the similar case studied in [ref] - [ref] .","intent_p":0.87,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":8,"sentences":9,"quotes":[{"arxiv_id":"1510.06760","title":"The charmonium dissociation in an \"anomalous wind\"","url":"/paper/1510.06760","section":"The screening length $l_s$ in the anomalous flow","sentence":"$l_0(η)$ are extensively discussed in literature [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"0809.5143","title":"Baryon Dissociation in a Strongly Coupled Plasma","url":"/paper/0809.5143","section":"Introduction and Conclusion","sentence":"This has resulted in some non-trivial progress in the understanding of screening phenomena in strongly coupled plasmas [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"0912.2238","title":"Light-like mesons and deep inelastic scattering in finite-temperature AdS/CFT with flavor","url":"/paper/0912.2238","section":"Introduction","sentence":"A substantial part of this effort has been concentrated on studying the response of such a plasma to energetic, `hard', probes, so like heavy quarks [ref] , mesons (or quark–antiquark pairs) [ref] , or photons [ref] , in an attempt to elucidate some intriguing RHIC data, so like the unexpectedly large `jet quenching', or to provide alternative signatures of a strongly–coupled matter.","intent_p":0.96,"contests_p":null},{"arxiv_id":"0710.5297","title":"Deep inelastic scattering off a N=4 SYM plasma at strong coupling","url":"/paper/0710.5297","section":"Introduction","sentence":"Following early applications to thermodynamics [ref] and the pioneering calculation, by Policastro, Son, and Starinets, of the shear viscosity [ref] , there was an intense activity towards computing the jet–quenching parameter [ref] , the energy–loss of a heavy quark [ref] or of a quark–antiquark pair [ref] , the diffusion rate for a heavy quark [ref] , the energy disturbances due to moving quarks [ref] , the Debye screening mass [ref] , the production rate for photons and dileptons [ref] , or the Bjorken expansion and the approach towards thermalization [ref] — all of that in the context of the strongly–coupled $𝒩=4$ SYM plasma at finite temperature (sometimes extended to include a chemical potential).","intent_p":0.96,"contests_p":null},{"arxiv_id":"0906.2964","title":"Holographic model with a NS-NS field","url":"/paper/0906.2964","section":"Meson in non-commutative QGP","sentence":"Such meson $qq̅$ in QGP has been extensively studied in [ref] - [ref] .","intent_p":0.95,"contests_p":null}]}],"unlabelled_sentences":22},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. 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