2007
DOI: 10.1088/0954-3899/34/8/s05
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Recent highlights from BRAHMS

Abstract: We present an overview of highlights from the BRAHMS Collaboration.

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Cited by 328 publications
(752 citation statements)
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“…6). For central Pb-Pb collisions at SPS energies, the typical results for transverse surface velocity and thermal freezeout temperature are (β s ⊥ /c, T fo [MeV]) = (0.65 ± 0.1, 120 ± 10) [79,80,81,82], which is quite comparable to the values used here for InIn. We emphasize that all contributions to the dilepton spectrum (QGP, ρ, ω, φ, and four-pion) are tied to the same evolution, thus fixing their relative weights.…”
Section: Thermal Fireball Evolutionsupporting
confidence: 76%
“…6). For central Pb-Pb collisions at SPS energies, the typical results for transverse surface velocity and thermal freezeout temperature are (β s ⊥ /c, T fo [MeV]) = (0.65 ± 0.1, 120 ± 10) [79,80,81,82], which is quite comparable to the values used here for InIn. We emphasize that all contributions to the dilepton spectrum (QGP, ρ, ω, φ, and four-pion) are tied to the same evolution, thus fixing their relative weights.…”
Section: Thermal Fireball Evolutionsupporting
confidence: 76%
“…For central heavy-ion (Au+Au or Pb+Pb) collisions at the AGS, SPS and RHIC accelerators, the approximate p T value at which the invariant cross sections of protons and positive pions at mid-rapidity approach each other is plotted. Data (with the percentile of most central events) are taken from the E802 [10] (4%), NA44 [11] (3.7%), NA49 [12] (5%), PHENIX [4,6] (5%) and PHOBOS (15%) experiments. A remarkably smooth collision energy dependence of the 'crossing' p T value is observed.…”
Section: Resultsmentioning
confidence: 99%
“…They are more precisely measurable than invariant cross sections, and provide quantitative input to models concentrating on the hadro-chemistry of the collisions, such as statistical thermal models. Antiproton to proton ratios and net proton yields provide information on baryon transport and baryon production in these ultrarelativistic collisions, and are relevant quantities to estimate the fraction of the total collision energy that is available for particle production [3].…”
Section: Introductionmentioning
confidence: 99%
“…These new solutions are simple, although their finding was a complicated process that lasted for decades. BRAHMS pointed out before [12], that the rapidity distribution of negative pions in Au+Au collisions at √ s N N = 200 GeV is flatter than a Gaussian, but not completely flat, hence neither the Landau-Khalatnikov, nor the Hwa-Bjorken solution describes it. Our new exact solutions describe well these BRAHMS observations.…”
Section: Relation To Earlier Solutionsmentioning
confidence: 99%