High Energy Physics - Theory · arXiv:1105.3384 v3 · submitted 17 May 2011
Calculating the jet quenching parameter in the plasma of NCYM theory from gauge/gravity duality
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“For small non-commutativity, we find that the value of the jet quenching parameter gets reduced from its commutative value.”
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Abstract
A particular decoupling limit of non-extremal (D1, D3) brane bound state system of type IIB string theory is known to give the gravity dual of space-space non- commutative Yang-Mills (NCYM) theory at finite temperature. We use a string probe in this background to compute the jet quenching parameter in the strongly coupled plasma of hot non-commutative Yang-Mills theory in (3+1)-dimensions from gauge/gravity duality. We give the expressions for the jet quenching parameter for both small and large non-commutativity. For small non-commutativity, we find that the value of the jet quenching parameter gets reduced from its commutative value. The reduction is enhanced with temperature as T^7 for fixed non-commutativity and the fixed 't Hooft coupling. We further generalize the results for the non-commutative Yang-Mills theories in diverse dimensions.
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abstract compiled · 2026-09-23 · no language-model review
How the main claim is stated: asserted 1.00
What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.10 · human participants 0.01 · controlled comparison 0.54 · randomized assignment 0.01 · states quantitative result 0.82 · compares with prior results 0.79 · mentions code or data availability 0.02
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This table labels the abstract only (arXiv listing abstract v3). The number is the probability the classifier gave the label.
| Sentence | Role | The authors' own work | States the main conclusion | Strength |
|---|---|---|---|---|
| A particular decoupling limit of non-extremal (D1, D3) brane bound state system of type IIB string theory is known to give the gravity dual of space-space non- commutative Yang-Mills (NCYM) theory at finite temperature. | background 1.00 | 0.05 | 0.03 | asserted 1.00 |
| We use a string probe in this background to compute the jet quenching parameter in the strongly coupled plasma of hot non-commutative Yang-Mills theory in (3+1)-dimensions from gauge/gravity duality. | contribution 0.75 | 0.95 | 0.11 | asserted 1.00 |
| We give the expressions for the jet quenching parameter for both small and large non-commutativity. | contribution 0.54 | 0.94 | 0.17 | asserted 0.99 |
| For small non-commutativity, we find that the value of the jet quenching parameter gets reduced from its commutative value. | result 1.00 | 0.96 | 0.41 | asserted 1.00 |
| The reduction is enhanced with temperature as T^{7} for fixed non-commutativity and the fixed 't Hooft coupling. | result 1.00 | 0.94 | 0.23 | asserted 1.00 |
| We further generalize the results for the non-commutative Yang-Mills theories in diverse dimensions. | contribution 0.97 | 0.90 | 0.07 | asserted 0.96 |
What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.95
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,993 input tokens, $0.0002 reported.
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How the literature uses it
5 arXiv papers cite this in 10 sentences
Papers citing it · 6 sentences without a confident label
Compares with it 1 paper
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Using this Wilson loop we obtained the expression of the jet quenching parameter in the NCYM theory which was obtained before [ref] using different approach.
Wilson loops in noncommutative Yang-Mills theory using gauge/gravity duality · Conclusion · 0.99
Cites it as background 2 papers
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Encouraged by the field-theoretical studies on anisotropic QGP [ref] , there have also been a spate of activities related to studying strongly coupled, anisotropic QGP via the gauge/string duality [ref] .
Drag force in strongly coupled, anisotropic plasma at finite chemical potential · Introduction · 0.86
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See [ref] , [ref] , [ref] , [ref] , [ref] , [ref] , [ref] for more recent works on the aforementioned decoupling and extension of the AdS/CFT to non-supersymmetric cases.
Application of top-down holographic thermal QCD at finite coupling · Generalization of AdS/CFT correspondence · 0.98
What it cites · 4 sentences without a confident label
Compares with 1 paper
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From [ref], we notice that when $θ=0$, we recover precisely the commutative result obtained in [ref] .
Wilson loops in (p+1)-dimensional Yang-Mills theories using gravity/gauge theory correspondence · Jet quenching for NCYM theories in other dimensions · 0.80
Cites as background 5 papers
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Jet quenching parameter [ref] , denoted by $q̂$, is a measure of the radiative parton energy loss when they interact strongly with the medium (the quark-gluon plasma or QGP), produced in the ultrarelativistic heavy ion collision (for example, Au-Au collision in RHIC or Pb-Pb collision in LHC), as they traverse through it (see, for example, [ref] for reviews on the subject). $q̂$ characterizes the properties of the medium and so by studying it one can gain insight about the properties of QCD matter in the extreme conditions as produced in the collision process.
Introductory lectures on jet quenching in heavy ion collisions · Introduction · 1.00
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Jet quenching parameter [ref] , denoted by $q̂$, is a measure of the radiative parton energy loss when they interact strongly with the medium (the quark-gluon plasma or QGP), produced in the ultrarelativistic heavy ion collision (for example, Au-Au collision in RHIC or Pb-Pb collision in LHC), as they traverse through it (see, for example, [ref] for reviews on the subject). $q̂$ characterizes the properties of the medium and so by studying it one can gain insight about the properties of QCD matter in the extreme conditions as produced in the collision process.
Radiative energy loss and $p_{\perp}$-broadening of high energy partons in nuclei · Introduction · 1.00
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Jet quenching in (3+1)-dimensional NCYM theory has also been considered recently in [ref] and [ref] .
Energy loss and jet quenching parameter in a thermal non-relativistic, non-commutative Yang-Mills plasma · Introduction · 0.97
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