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Dilepton and Photon Emission Rates from a Hadronic Gas II
High Energy Physics - Phenomenology · Submitted 28 Apr 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The opening of the $\pi N$ cut causes the photon rate to saturate the empirical photon yield of WA80, but may not be enough to fully account for the excess low mass dileptons seen at CERES.
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The abstract, sentence by sentence
We extend our recent analysis of the dilepton and photon emission rates to the case of finite temperature and baryon density, within the context of a density expansion. To leading order, the effects of the baryon density are assessed using data (photon emission) or constraints from broken chiral symmetry (dilepton emission). Next to leading order effects are worked out, and their contribution qualitatively assessed. The opening of the $\pi N$ cut causes the photon rate to saturate the empirical photon yield of WA80, but may not be enough to fully account for the excess low mass dileptons seen at CERES.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We extend our recent analysis of the dilepton and photon emission rates to the case of finite temperature and baryon density, within the context of a density expansion. | contribution 0.99 | 0.88 | 0.07 | asserted 0.96 |
| s1 | To leading order, the effects of the baryon density are assessed using data (photon emission) or constraints from broken chiral symmetry (dilepton emission). | method 0.96 | 0.58 | 0.07 | asserted 1.00 |
| s2 | Next to leading order effects are worked out, and their contribution qualitatively assessed. | contribution 0.85 | 0.92 | 0.06 | asserted 0.92 |
| s3 | The opening of the $\pi N$ cut causes the photon rate to saturate the empirical photon yield of WA80, but may not be enough to fully account for the excess low mass dileptons seen at CERES. | result 0.77 | 0.74 | 0.68 | hedged possibility 0.84 |
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The paper
Original abstract
We extend our recent analysis of the dilepton and photon emission rates to the case of finite temperature and baryon density, within the context of a density expansion. To leading order, the effects of the baryon density are assessed using data (photon emission) or constraints from broken chiral symmetry (dilepton emission). Next to leading order effects are worked out, and their contribution qualitatively assessed. The opening of the $\pi N$ cut causes the photon rate to saturate the empirical photon yield of WA80, but may not be enough to fully account for the excess low mass dileptons seen at CERES.
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How the literature uses it
4 arXiv papers cite this in 7 sentences
Papers citing it · 5 sentences without a confident label
Uses its method or tool 1 paper
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Below $T_c$ we use the rate equations presented in [ref] for a hadronic gas at finite temperature and Baryon density which are constrained entirely by broken chiral symmetry:
Low mass dilepton radiation at RHIC · Dilepton Rates · 0.96
Compares with it 1 paper
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In the intermediate mass region, our rates favor the current upper bounds from the data and is consistent with a previous analysis using $W_π$ and the baryon contributions [ref] .
Dileptons and Photons at RHIC · SPS · 0.84
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