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Thermal dilepton production from hot QCD
High Energy Physics - Phenomenology · Submitted 20 Feb 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim An interpolation applicable for all positive photon invariant masses is presented, and possibilities for comparisons with lattice and experimental data are pointed out.
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The abstract, sentence by sentence
NLO and LPM-resummed computations of thermal dilepton production from a hot QCD plasma are reviewed. An interpolation applicable for all positive photon invariant masses is presented, and possibilities for comparisons with lattice and experimental data are pointed out.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | NLO and LPM-resummed computations of thermal dilepton production from a hot QCD plasma are reviewed. | contribution 0.58 | 0.16 | 0.12 | asserted 0.88 |
| s1 | An interpolation applicable for all positive photon invariant masses is presented, and possibilities for comparisons with lattice and experimental data are pointed out. | contribution 0.93 | 0.84 | 0.35 | asserted 0.54 |
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The paper
Original abstract
NLO and LPM-resummed computations of thermal dilepton production from a hot QCD plasma are reviewed. An interpolation applicable for all positive photon invariant masses is presented, and possibilities for comparisons with lattice and experimental data are pointed out.
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3 arXiv papers cite this in 3 sentences
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Uses its method or tool 1 paper
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Using the Fermi-Dirac distribution $f(p)=1/(e^p/T+1)$ for $f_q$ and $f_q̅$, where $T$ is the temperature of the plasma, the remaining integral over $p_1$ can be carried out analytically [ref] , and one obtains: [equation] where [equation] is a correction factor that reduces to unity in the limit where $k^0≫T$ and $k^0≫k$.
Intermediate mass dileptons as pre-equilibrium probes in heavy ion collisions · Dilepton production in a non-equilibrium QGP · 0.91
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